Physics skims

21.2. Physics skims#

21.2.1. B → charm skims#

List of functions to skim events containing \(B\to X_c + h\) decays, where \(X_c\) stands for \(D^0\), \(D^{\pm}\), \(D^{*0}\) and \(D^{*\pm}\), and \(h\) stands for \(\pi^{\pm}\), \(K^{\pm}\), \(\rho^{\pm}\) and \(a_1^{\pm}\).

class skim.WGs.btocharm.B0toD0Kpipi0_pi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toD0Kpipi0_pi0
Skim LFN code: 14121300
Category: physics, hadronic B to charm
Author: Francis Pham
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \overline{D}{}^{0} (\to K^+ \pi^- \pi^0) \pi^0\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.5

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpipi0, where the \(\overline{D}{}^{0}\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDD_Kpipi_Kspi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDD_Kpipi_Kspi
Skim LFN code: 14141002
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{+}(\to K^- \pi^+ \pi^+) D^{-}(\to K^+ \pi^- \pi^-)\)
\(B^{0}\to D^{+}(\to K^- \pi^+ \pi^+) D^{-}(\to K_{\rm S}^0 \pi^-)\)
\(B^{0}\to D^{+}(\to K_{\rm S}^0 \pi^-) D^{-}(\to K_{\rm S}^0 \pi^-)\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3
1.8 < M_D < 1.9

Note

This skim uses skim.standardlists.charm.loadStdDplus_Kpipi and skim.standardlists.charm.loadStdDplus_Kspi, where \(D^-\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDDs0star(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDDs0star
Skim LFN code: 14160201
Category: physics, hadronic B to charm
Author: Kuanying Wu
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D_{s0}^{*+} (\to D_{s}^{+} (\to \phi (\to K^+ K^-) \pi^+ \pi^0) \pi^0) D^{-} (\to K^+ \pi^- \pi^-)\)
\(B^{0}\to D_{s0}^{*+} (\to D_{s}^{+} (\to \overline{K}{}^{*0} (\to K^- \pi^+ ) K^+) \pi^0) D^{-} (\to K^+ \pi^- \pi^-)\)
\(B^{0}\to D_{s0}^{*+} (\to D_{s}^{+} (\to \phi (\to K^+ K^-) \pi^+) \pi^0) D^{-} (\to K^+ \pi^- \pi^-)\)

Cuts applied:

5.2 < Mbc < 5.3
abs(deltaE) < 0.2
0.31 < D_s0ST_massDifference_0 < 0.347

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.B0toDomegapi_Kpipi_pipipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDomegapi_Kpipi_pipipi0
Skim LFN code: 14141701
Category: physics, hadronic B to charm
Author: Dmitry Matvienko
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0} \to D^{-} (\to K^+ \pi^- \pi^-) \omega (\to \pi^- \pi^+ \pi^0) \pi^+\),

Cuts applied:

1.84 < M_D < 1.90
0.70 < M_omega < 0.90
Mbc > 5.25
abs(deltaE) < 0.25

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDomegapi_Kspi_pipipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDomegapi_Kspi_pipipi0
Skim LFN code: 14141702
Category: physics, hadronic B to charm
Author: Dmitry Matvienko
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0} \to D^{-} (\to K_{\rm S}^0 \pi^-) \omega (\to \pi^- \pi^+ \pi^0) \pi^+\),

Cuts applied:

1.84 < M_D < 1.90
0.70 < M_omega < 0.90
Mbc > 5.25
abs(deltaE) < 0.25

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDpi_Kpipi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDpi_Kpipi
Skim LFN code: 14120600
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{-} (D^{0} \to K^+ \pi^- \pi^-) \pi^+\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdDplus_Kpipi, where \(D^-\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDpi_KpipiLooseDelE(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDpi_KpipiLooseDelE
Skim LFN code: 14120602
Category: physics, hadronic B to charm
Author: Sourav Dey
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{-} (D^{0} \to K^+ \pi^- \pi^-) \pi^+\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.45

Note

This skim is the same as B0toDpi_Kpipi, with the only difference of a larger deltaE cut (abs(deltaE) < 0.45). As for B0toDpi_Kpipi, this skim uses skim.standardlists.charm.loadStdDplus_Kpipi, where \(D^0\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDpi_Kspi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDpi_Kspi
Skim LFN code: 14120601
Category: physics, hadronic B to charm
Authors: Fernando Abudinen, Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{-} (\to K_{\rm S}^0 \pi^-) \pi^+\),

Cuts applied:

1.8 < M_D < 1.9
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses stdV0s.stdKshorts and skim.standardlists.charm.loadStdDplus_Kpipi, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDrho_Kpipi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDrho_Kpipi
Skim LFN code: 14121100
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{-} (\to K^+ \pi^- \pi^-) \rho^+\),

Cuts applied:

1.8 < M_D < 1.9
0.47 < M_rho < 1.07
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdDplus_Kpipi, where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDrho_Kspi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDrho_Kspi
Skim LFN code: 14121101
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{-} (\to K_{\rm S}^0 \pi^-) \rho^+\),

Cuts applied:

1.8 < M_D < 1.9
0.47 < M_rho < 1.07
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses stdV0s.stdKshorts and skim.standardlists.charm.loadStdDplus_Kspi, where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDs1D(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDs1D
Skim LFN code: 14160200
Category: physics, hadronic B to charm
Author: Tsai Hua Lee, Chih Han Tseng
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D_{s1}^{+} (\to D_s^{*+}(\to D_s^+(\to \phi (\to K^+ K^-)\pi^+) \gamma) \pi^0) D^- (\to K^+ \pi^-\pi^-)\),
\(B^{0}\to D_{s1}^{+} (\to D_s^{*+}(\to D_s^+(\to \phi (\to K^+ K^-) \pi^+ \pi^0) \gamma) \pi^0) D^- (\to K^+ \pi^-\pi^-)\),
\(B^{0}\to D_{s1}^{+} (\to D_s^{*+}(\to D_s^+(\to \overline{K}{}^{*0} (\to K^- \pi^+)K^+) \gamma) \pi^0) D^- (\to K^+ \pi^-\pi^-)\),
\(B^{0}\to D_{s1}^{+} (\to D_s^{*+}(\to D_s^+(\to K_S^0 (\to \pi^- \pi^+)K^+) \gamma) \pi^0) D^- (\to K^+ \pi^-\pi^-)\),

Cuts applied:

5.2 < Mbc < 5.3
-0.5 < deltaE < 0.5
0.247 < M(D_s1+) - M(D_s*+) < 0.378
0.072 < M(D_s*+) - M(D_s+) < 0.179
2.288 < M(D_s1+) < 2.507

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.B0toDstarD(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarD
Skim LFN code: 14141003
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \overline{D}{}^{*-} (\to \overline{D}{}^{0} (\to K^+ \pi^-, \to K^+ \pi^- \pi^- \pi^+, K^+ \pi^- \pi^0) \pi^-) D^+ (\to K^- \pi^+ \pi^+)\)
\(B^{0}\to \overline{D}{}^{*-} (\to D^{-} \pi^0) D^+ (\to K^- \pi^+ \pi^+)\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3
DM_Dstar_D < 0.16
1.8 < M_D < 1.9

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDstarPi_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarPi_D0pi_Kpi
Skim LFN code: 14120700
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^-) \pi^+\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpi, where the \(D^{*-}\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDstarPi_D0pi_Kpipipi_Kpipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarPi_D0pi_Kpipipi_Kpipi0
Skim LFN code: 14120800
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \overline{D}{}^{*-} (\to \overline{D}{}^{0} (\to K^+ \pi^- \pi^- \pi^+, K^+\pi^-\pi^0) \pi^-) \pi^+\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDstarRho_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarRho_D0pi_Kpi
Skim LFN code: 14121200
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{*-} (\to \overline{D}{}^{0} (\to K^+ \pi^-) \pi^-) \rho^+\),

Cuts applied:

1.7 < M_D < 2.0
0.47 < M_rho < 1.07
DM_Dstar_D < 0.16
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi and skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpi where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDstarRho_D0pi_Kpipipi_Kpipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarRho_D0pi_Kpipipi_Kpipi0
Skim LFN code: 14121201
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to D^{*-} (\to \overline{D}{}^{0} (\to K^+2\pi^-\pi^+, K^+\pi^-\pi^0)\pi^-) \rho^+\),

Cuts applied:

1.7 < M_D < 2.0
0.47 < M_rho < 1.07
DM_Dstar_D < 0.16
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpipi0, skim.standardlists.charm.loadStdD0_Kpipipi, skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpipi0 and skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpipipi where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.btocharm.B0toDstaretapi_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstaretapi_D0pi_Kpi
Skim LFN code: 14121500
Category: physics, hadronic B to charm
Author: Vismaya V S
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \overline{D}^{*-} (\to \bar{D}^{0} (\to K^+ \pi^-) \pi^-) \eta (\to \gamma \gamma) \pi^+\)

Cuts applied:

Mbc > 5.25
abs(deltaE) < 0.32
1.7 < M_D0 < 2.0
(M_D* - M_D0) < 0.16
0.35 < M_eta < 0.7
Energy_photons > 0.05

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi and skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpi, where the \(\bar{D}^{0}\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.B0toDstarpipi0_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarpipi0_D0pi_Kpi
Skim LFN code: 14121400
Category: physics, hadronic B to charm
Author: Vismaya V S
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \overline{D}^{*-} (\to \bar{D}^{0} (\to K^+ \pi^-) \pi^-) \pi^+ \pi^0\)

Cuts applied:

Mbc > 5.25
abs(deltaE) < 0.32
1.7 < M_D < 2.0
(M_D* - M_D0) < 0.16

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi and skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpi, where the \(\bar{D}^{0}\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BptoD0etapi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BptoD0etapi_Kpi
Skim LFN code: 14121600
Category: physics, hadronic B to charm
Author: Vismaya V S
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \bar{D}^{0} (\to K^+ \pi^-) \eta (\to \gamma \gamma) \pi^+\)

Cuts applied:

Mbc > 5.25
abs(deltaE) < 0.32
1.7 < M_D < 2.0
0.35 < M_eta < 0.7
E_photons > 0.05

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BptoD0pipi0_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BptoD0pipi0_Kpi
Skim LFN code: 14121601
Category: physics, hadronic B to charm
Author: Vismaya V S
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \bar{D}^{0} (\to K^+ \pi^-) \pi^+ \pi^0\)

Cuts applied:

Mbc > 5.25
abs(deltaE) < 0.32
1.7 < M_D < 2.0

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoD0h_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_Kpi
Skim LFN code: 14140101
Category: physics, hadronic B to charm
Author: Niharika Rout
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Skim list definitions for all charged B to charm 3 body decays.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^-) K^+\),

Cuts applied:

1.7 < M_D0 < 2.0
Mbc > 5.2
abs(deltaE) < 0.5

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoD0h_Kpipipi_Kpipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_Kpipipi_Kpipi0
Skim LFN code: 14140102
Category: physics, hadronic B to charm
Author: Chiara La Licata
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^- \pi^- \pi^+, \to K^+ \pi^- \pi^0) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^- \pi^- \pi^+, \to K^+ \pi^- \pi^0) K^+\),
\(B^{+}\to \overline{D}{}^{*0} (\to \overline{D}{}^{0} (\to K^+2\pi^-\pi^+, K^+\pi^-\pi^0) \pi^0) \pi^+\)
\(B^{+}\to \overline{D}{}^{*0} (\to \overline{D}{}^{0} (\to K^+2\pi^-\pi^+, K^+\pi^-\pi^0) \pi^0) K^+\)

Cuts applied:

1.7 < M_D0 < 2.0
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpipipi and skim.standardlists.charm.loadStdD0_Kpipi0, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoD0h_Kshh(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_Kshh
Skim LFN code: 14140200
Category: physics, hadronic B to charm
Author: Minakshi Nayak
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^+ \pi^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^- \pi^+) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^+ \pi^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^+ K^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^+ \pi^-) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^- \pi^+) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^+ \pi^-) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 K^+ K^-) K^+\),

Cuts applied:

1.5 < M_D0 < 2.2
5.2 < Mbc
deltaE < 0.3 and deltaE > -0.45

Note

This skim uses skim.standardlists.charm.loadD0_Kshh_loose, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.BtoD0h_Kspi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_Kspi0
Skim LFN code: 14120300
Category: physics, hadronic B to charm
Author: Minakshi Nayak
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^0) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^0) K^+\),

Cuts applied:

1.5 < M_D0 < 2.2
5.2 < Mbc
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadD0_Kspi0_loose, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.BtoD0h_Kspipipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_Kspipipi0
Skim LFN code: 14120400
Category: physics, hadronic B to charm
Author: Niharika Rout
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^+ \pi^- \pi^0) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K_{\rm S}^0 \pi^+ \pi^- \pi^0) K^+\),

Cuts applied:

1.8 < M_D0 < 1.9
5.25 < Mbc
abs(deltaE) < 0.2

Note

This skim uses skim.standardlists.charm.loadD0_Kspipipi0, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.BtoD0h_hh(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0h_hh
Skim LFN code: 14140100
Category: physics, hadronic B to charm
Author: Hulya Atmacan
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Skim list definitions for all charged B to charm 2 body decays.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^- \pi^+) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to \pi^+ \pi^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^+ K^-) \pi^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^-) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^- \pi^+) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to \pi^+ \pi^-) K^+\),
\(B^{+}\to \overline{D}{}^{0} (\to K^+ K^-) K^+\),

Cuts applied:

1.5 < M_D0 < 2.2
5.2 < Mbc
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadD0_hh_loose, where \(D^0\) channels are defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.BtoD0pi_Kpiomega_pipipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0pi_Kpiomega_pipipi0
Skim LFN code: 14141703
Category: physics, hadronic B to charm
Author: Dmitry Matvienko
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+} \to \bar{D}^{0} (\to K^+ \pi^- \omega (\to \pi^- \pi^+ \pi^0)) \pi^+\),

Cuts applied:

1.7 < M_D < 2.0
0.73 < M_omega < 0.9
Mbc > 5.25
abs(deltaE) < 0.25

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoD0rho_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0rho_Kpi
Skim LFN code: 14141000
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K^+ \pi^-) \rho^+\),
\(B^{+}\to \overline{D}{}^{*0} (\to \overline{D}{}^{0} (\to K^+ \pi^-) \pi^0) \rho^+\),

Cuts applied:

1.7 < M_D0 < 2.0
0.47 < M_rho < 1.07
DM_Dstar_D < 0.16
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi and skim.standardlists.charm.loadStdDstar0_D0pi0_Kpi, where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoD0rho_Kpipipi_Kpipi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoD0rho_Kpipipi_Kpipi0
Skim LFN code: 14141001
Category: physics, hadronic B to charm
Author: Fernando Abudinen
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to \overline{D}{}^{0} (\to K^+2\pi^-\pi^+, K^+\pi^-\pi^0) \rho^+\)
\(B^{+}\to \overline{D}{}^{*0} (\to \overline{D}{}^{0} (\to K^+2 \pi^- \pi^+, K^+\pi^-\pi^0) \pi^0) \rho^+\)

Cuts applied:

1.7 < M_D0 < 2.0
DM_Dstar_D < 0.16
0.6 < M_rho < 0.9
cosHel_rho < 0.90
Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpipi0, skim.standardlists.charm.loadStdD0_Kpipipi, skim.standardlists.charm.loadStdDstar0_D0pi0_Kpipi0, and skim.standardlists.charm.loadStdDstar0_D0pi0_Kpipipi, where \(D^0\) channels are defined, and skim.standardlists.lightmesons.loadStdAllRhoPlus.

Warning

This skim saves only three randomly-chosen \(B^{+}\) candidates in a B+:BtoD0rho_merged list, since the candidate multiplicity of this skim is very high.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoDpipi_Kpipi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoDpipi_Kpipi
Skim LFN code: 14121402
Category: physics, hadronic B to charm
Author: Melisa-Melek Akdag
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{-}\to D^{+} (\to K^- \pi^+ \pi^-) \pi^- \pi^-\),

Cuts applied:

5.22 < Mbc
-0.3 < deltaE < 0.2

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.BtoDsDsst_Kpi_KK(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoDsDsst_Kpi_KK
Skim LFN code: 14121403
Category: physics, hadronic B to charm
Author: Agrim Aggarwal
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to D_{s}^{-} (\to \phi (\to K^+ K^-) \pi^+) K^+ \pi^+\),
\(B^{+}\to D_{s}^{-} (\to K^{*0} (\to K^- \pi^+) K^-) K^+ \pi^+\),
\(B^{+}\to D_{s}^{-} (\to K_{\rm S}^0 (\to \pi^+ \pi^-) K^-) K^+ \pi^+\),
\(B^{+}\to D_{s}^{-} (\to \phi (\to K^+ K^-) \pi^+) K^+ K^+\),
\(B^{+}\to D_{s}^{-} (\to K^{*0} (\to K^- \pi^+) K^-) K^+ K^+\),
\(B^{+}\to D_{s}^{-} (\to K_{\rm S}^0 (\to \pi^+ \pi^-) K^-) K^+ K^+\),
\(B^{+}\to D_{s}^{*-} (\to D_{s}^{-} \gamma ) K^+ \pi^+\),
\(B^{+}\to D_{s}^{*-} (\to D_{s}^{-} \gamma ) K^+ K^+\),

Cuts applied:

5.24 < Mbc
-0.2 < deltaE < 0.2
0.82 < M_K*0 < 0.98
1.93 < M_Ds < 1.99
2.06 < M_D*s < 2.15

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoDstarpipipi0_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoDstarpipipi0_D0pi_Kpi
Skim LFN code: 14161400
Category: physics, hadronic B to charm
Author: Fedja Ceplak Mencin
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{+}\to D^{*-} (\to \overline{D}^{0} (\to K^+ \pi^-) \pi^-) \pi^+ \pi^+ \pi^0\)

Cuts applied:

Mbc > 5.2
abs(deltaE) < 0.3

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpi and skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpi, where \(D^{*-}\) channel is defined.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharm.BtoDstpipi_D0pi_Kpi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BtoDstpipi_D0pi_Kpi
Skim LFN code: 14121401
Category: physics, hadronic B to charm
Author: Agrim Aggarwal
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{-}\to D^{*+} (\to D^0 (\to K^+ \pi^-) \pi^+) \pi^- \pi^-\),

Cuts applied:

5.22 < Mbc
-0.3 < deltaE < 0.2

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.antiB0toDpipi0_Kpipi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: antiB0toDpipi0_Kpipi
Skim LFN code: 14123300
Category: physics, hadronic B to charm
Author: Agrim Aggarwal
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(\bar{B^{0}}\to D^{+} (\to K^- \pi^+ \pi^-) \pi^- \pi^0\),

Cuts applied:

5.22 < Mbc
-0.3 < deltaE < 0.2

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.btocharm.antiB0toDsDsst_Kpi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: antiB0toDsDsst_Kpi0
Skim LFN code: 14163400
Category: physics, hadronic B to charm
Author: Agrim Aggarwal
Contact: Yi Zhang

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(\bar{B^{0}}\to D_{s}^{+} (\to \phi (\to K^+ K^-) \pi^+) K^- \pi^0\),
\(\bar{B^{0}}\to D_{s}^{+} (\to K^{*0} (\to K^- \pi^+) K^-) K^- \pi^0\),
\(\bar{B^{0}}\to D_{s}^{+} (\to K_{\rm S}^0 (\to \pi^+ \pi^-) K^-) K^- \pi^0\),
\(\bar{B^{0}}\to D_{s}^{*+} (\to D_{s}^{-} \gamma ) K^- \pi^0\),

Cuts applied:

5.24 < Mbc
-0.2 < deltaE < 0.2
0.82 < M_K*0 < 0.98
1.93 < M_Ds < 1.99
2.06 < M_D*s < 2.15

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

21.2.2. B → charmless skims#

Skim list building functions for \(B\to X_u +h\) analyses

class skim.WGs.btocharmless.BtoEtapKstp(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for B+ to eta’ K*+.
Skim name: BtoEtapKstp
Skim LFN code: 19140500
Category: physics, hadronic B to charmless
Author: Chia-Ling Hsu
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay mode:

\(B^{+}\to \eta^{'} K^{*+}\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5
0.4 < M_{eta} < 0.6
0.8 < M_{eta'} < 1.1
0.7 < M_{K*} < 1.6

Note

This skim uses skim.standardlists.lightmesons.loadStdSkimHighEffEtaPrime and skim.standardlists.charmless.loadStdVeryLooseKstarPlus where \(\eta^{'}\) and \(K^{*+}\) are defined, respectively. \(\eta\) channel is defined in skim.standardlists.lightmesons.loadStdSkimHighEffEta.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoEtapRhop(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for B+ to etap rho+.
Skim name: BtoEtapRhop
Skim LFN code: 19140200
Category: physics, hadronic B to charmless
Author: Ruei-Si Hsiao
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay mode:

\(B^{+}\to \eta^{'} (\to \pi^{+} \pi^{-} \eta (\to \gamma \gamma) ) \rho^{+} (\pi^{+} \pi^{0})\)
\(B^{+}\to \eta^{'} (\to \rho^{0} (\to \pi^{+} \pi^{-}) \gamma ) \rho^{+} (\pi^{+} \pi^{0})\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5
0.8< M_{etap} < 1.1
0.4< M_{eta} < 0.6
0.47 < M_{rhop} < 1.15
0.47 < M_{rho0} < 1.15

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoHad1Pi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for B to charmless modes including 1 pi0 in the final state.
Skim name: BtoHad1Pi0
Skim LFN code: 19130300
Category: physics, hadronic B to charmless
Authors: Fernando Abudinen, Riccardo Manfredi, Sebastiano Raiz, Benedikt Wach
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^+\to \pi^+ \pi^0\)
\(B^+\to K^+ \pi^0\)
\(B^0\to \pi^+ \pi^- \pi^0\)
\(B^0\to K^+ \pi^- \pi^0\)
\(B^0\to K^- \pi^+ \pi^0\)
\(B^0\to K^+ K^- \pi^0\)
\(B^0\to K_{\rm S}^0 \pi^0\)
\(B^+\to K_{\rm S}^{0} \pi^+ \pi^0\)
\(B^+\to K_{\rm S}^{0} K^+ \pi^0\)
\(B^+\to \rho^{+} \rho^{0}\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoHad3Tracks1Pi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for all charged B to charmless modes with 3 tracks and 1 Pi0.
Skim name: BtoHad3Tracks1Pi0
Skim LFN code: 19130310
Category: physics, hadronic B to charmless
Authors: Fernando Abudinen, Riccardo Manfredi, Sebastiano Raiz, Benedikt Wach
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^+\to K^{*+} K^+ K^-\)
\(B^+\to K^{*+} K^+ \pi^-\)
\(B^+\to K^{*+} \pi^+ \pi^-\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoHadTracks(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list definitions for all B to charmless modes with tracks only in the final state.
Skim name: BtoHadTracks
Skim LFN code: 19130201
Category: physics, hadronic B to charmless
Authors: Fernando Abudinen, Riccardo Manfredi, Sebastiano Raiz, Benedikt Wach
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^{0}\to \pi^+ \pi^-\)
\(B^{0}\to K^+ \pi^-\)
\(B^{0}\to K^+ K^-\)
\(B^{+}\to \pi^+ \pi^+ \pi^-\)
\(B^{+}\to K_{\rm S}^0 \pi^+\)
\(B^{+}\to K_{\rm S}^0 K^+\)
\(B^{+}\to K^+ \pi^+ \pi^-\)
\(B^{+}\to K^+ K^+ \pi^-\)
\(B^{+}\to K^+ K^- \pi^+\)
\(B^{+}\to K^+ K^+ K^-\)
\(B^{0}\to \pi^+ \pi^- \pi^+ \pi^-\)
\(B^{0}\to K^+ \pi^- \pi^+ \pi^-\)
\(B^{0}\to K^+ K^- \pi^+ \pi^-\)
\(B^{0}\to K^+ \pi^- K^+ \pi^-\)
\(B^{0}\to K^+ K^- K^+ \pi^-\)
\(B^{0}\to K^+ K^- K^+ K^-\)
\(B^{0}\to K_{\rm S}^0 \pi^+ \pi^-\)
\(B^{0}\to K_{\rm S}^0 K^+ \pi^-\)
\(B^{0}\to K_{\rm S}^0 K^+ K^-\)
\(B^{0}\to K_{\rm S}^0 K_{\rm S}^0\)
\(B^{0}\to K^{*0} K^- K^+\)
\(B^{0}\to K^{*0} \pi^- \pi^+\)
\(B^{0}\to K^{*0} K^+ \pi^-\)
\(B^{0}\to \rho^0 \rho^0\)
\(B^{+}\to K^{*+} K^- K^+\)
\(B^{+}\to K^{*+} \pi^- \pi^+\)
\(B^{+}\to K^{*+} K^+ \pi^-\)

Cuts applied:

nTracks >= 2 (event level)
5.20 < Mbc < 5.29
abs(deltaE) < 0.3

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoPi0Eta(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list definitions for neutral B to pi0 eta and B to pi0 eta’.
Skim name: BtoPi0Eta
Skim LFN code: 19130600
Category: physics, hadronic B to charmless
Authors: Longke Li, Yinghui Guan
Contact: Benedikt Wach

Reconstructed decay modes:

\(B^{0}\to \pi^0 \eta\)
\(B^{0}\to \pi^0 \eta^{'}\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoPi0Pi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list definitions for neutral B to two neutral pions.
Skim name: BtoPi0Pi0
Skim LFN code: 19120100
Category: physics, hadronic B to charmless
Authors: Fernando Abudinen, Riccardo Manfredi, Sebastiano Raiz, Francis Pham, Benedikt Wach
Contact: Benedikt Wach

Reconstructed decay modes:

\(B^{0}\to \pi^0 \pi^0\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.btocharmless.BtoRhopRhom(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for B to rho+ rho-.
Skim name: BtoRhopRhom
Skim LFN code: 19120400
Category: physics, hadronic B to charmless
Authors: Yu Nakazawa, Benedikt Wach
Contact: Benedikt Wach

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^+ \to \rho^{+} \rho^{-}\)

Cuts applied:

5.20 < Mbc < 5.29
abs(deltaE) < 0.5

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

21.2.3. Charm physics skims#

Skim list building functions for charm analyses.

Note

The Hp, Hm and Jm in the function name represent arbitrary charged particles with positive or negative charge. The Hp and Jm in XToD0_D0ToHpJm, mean a positive particle and a negative particle that could be either conjugate or non-conjugate. The Hp and Hm in EarlyData_DstToD0Pi_D0ToHpHmPi0, mean a positive particle and a negative particle that must be conjugate.

Note

Although reconstructDecay() would automatically include charged conjugate channel, and D0 is not distinguishable from anti-D0 in XToD0 skim, both \(D^0 \to f\) and \(D^0 \to \overline{f}\) mode should be written explicitly in XToD0 skim, because later in the DstToD0Pi skim, the D0 decay strings in XToD0 skim would be directly combined with pi+. For example, if one only include D0 -> K+ pi- in XToD0_D0ToHpJm skim, then in DstToD0Pi_D0ToHpJm skim, only the D*+ -> [D0 -> K+ pi-] pi+ would be included, and D*+ -> [D0 -> K- pi+] pi+ would not be included.

class skim.WGs.charm.DpToEtaHp(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to eta h+
Skim name: DpToEtaHp
Skim LFN code: 17241300
Category: physics, charm
Author: Jaeyoung Kim
Contact: Jaeyoung Kim

Decay Modes:

\(D^{+}\to \eta \pi^+\) (and CC)
\(D^{+}\to \eta \K^+\) (and CC)

Selection Criteria:

Track cuts are charm_skim_std_charged pion and Kaon
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
\(0.4 < M(\eta_{\gamma\gamma} < 0.6\)
\(0.48 < M(\eta_{\pi^{+}\pi^{-}\pi^{0}} < 0.6\)
\(p(\eta) > 0.4\)
\(1.6 < M(D^{+}) < 2.1\)
\(p*(D^{+})>2.2\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DpToHpOmega(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to h+ omega, omega to pi+ pi- pi0.
Skim name: DpToHpOmega
Skim LFN code: 17260100
Category: physics, charm
Author: Yongheon Ahn
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{+}\to K^{+} \omega\) (and CC)
\(D^{+}\to \pi^+ \omega\) (and CC)
\(\omega\to \pi^+ \pi^- \pi^0\)

Selection Criteria:

Track cuts are charm_skim_std_charged pion and Kaon with PID > 0.1
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
p(pi0) > 0.25 and 0.11 < InvM(pi0) < 0.15
0.71 < M(omega) < 0.85
1.67 < M(D+) < 2.07
p*(D+) > 2.0

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DpToHpPi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to h+ pi0 without D* tag.
Skim name: DpToHpPi0
Skim LFN code: 17232000
Category: physics, charm
Author: Yifan Jin
Contact: Jaeyoung Kim

Decay Modes:

\(D^+ \to \pi^+ \pi^0\)

Selection Criteria:

Tracks: dr < 1, abs(dz) < 3, thetaInCDCAcceptance, pcms(\pi^{+}) > 0.5
Use \(\pi^{0}\) from stdPi0s require pcms(\pi^{0}) > 0.5
1.57 < M(D+) < 2.17, pcms(D+) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DpToPipEpEm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to pi+ e+ e-.
Skim name: DpToPipEpEm
Skim LFN code: 17220100
Category: physics, charm
Author: Andrej Lozar
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^+ \to \pi^+ e^- e^+\),

Selection Criteria:

Use tracks from the charm lists in charm_skim_std_charged
1.67 < M(D+) < 2.17, pcms(D+) > 2.0 and loose cuts for ee
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DpToPipKpKm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to pi+ K+ K-.
Skim name: DpToPipKpKm
Skim LFN code: 17220300
Category: physics, charm
Author: Andrej Lozar
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^+ \to \pi^+ K^- K^+\)

Selection Criteria:

Use tracks from the charm lists in charm_skim_std_charged
1.67 < M(D+) < 2.17, pcms(D+) > 2.0 and loose cuts for KK
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DpToPipMupMum(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D+ to pi+ mu+ mu-.
Skim name: DpToPipMupMum
Skim LFN code: 17220200
Category: physics, charm
Author: Andrej Lozar
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^+ \to \pi^+ \mu^- \mu^+\)

Selection Criteria:

Use tracks from the charm lists in charm_skim_std_charged
1.67 < M(D+) < 2.17, pcms(D+) > 2.0 and loose cuts for mumu
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DspToHpOmega(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D_s+ to h+ omega, omega to pi+ pi- pi0.
Skim name: DspToHpOmega
Skim LFN code: 17260200
Category: physics, charm
Author: Yongheon Ahn
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D_{s}^{+}\to K^{+} \omega\) (and CC)
\(D_{s}^{+}\to \pi^+ \omega\) (and CC)
\(\omega\to \pi^+ \pi^- \pi^0\)

Selection Criteria:

Track cuts are charm_skim_std_charged pion and Kaon with PID > 0.1
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
p(pi0) > 0.25 and 0.11 < InvM(pi0) < 0.15
0.71 < M(omega) < 0.85
1.77 < M(D_s+) < 2.17
p*(D_s+) > 2.0

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToGeneric(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for Inclusive D0 from charm tagger
Skim name: DstToD0Pi_D0ToGeneric
Skim LFN code: 17230700
Category: physics, charm
Author: Chanho Kim
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to D^{0} \pi^{+}\) (signal side)
\(D^{*+}\to D^0 \pi^{+}\) and \(D^{*+}\to D^{+} \pi^{0}\) (tag side)
\(D^{*0}\to D^0 \pi^{0}\) and \(D^{*0}\to D^{0} \gamma\) (tag side)
\(D_s^{*+}\to D_s^{+} \gamma\) (tag side)
15 hadronic channels for tag \(D^{0}\) reconstruction
11 hadronic channels for tag \(D^{+}\) reconstruction
10 hadronic channels for tag \(D_{s}^{+}\) reconstruction
19 hadronic channels for tag \(\Lambda_{c}^{+}\) reconstruction

Selection Criteria:

Cut on \(\pi^{+}, K^{+}\) : charm_skim_std_charged pion and kaon with PIDNN > 0.1
Cut on \(p^{+}\) : abs(dr) < 1.0 and abs(dz) < 3.0 and protonID > 0.1
Cut on \(\gamma\) : E > 0.05
Cut on \(\pi^{0}\to \gamma \gamma\) : 0.115 < M < 0.160
Cut on tag side \(D^{0}\) : 1.72 < M < 2.02 and p* > 2.0
Cut on tag side \(D^{+}\) : 1.72 < M < 2.02 and p* > 2.0
Cut on tag side \(D_{s}^{+}\) : 1.82 < M < 2.12 and p* > 2.0
Cut on tag side \(\Lambda_{c}^{+}\) : 2.18 < M < 2.38 and p* > 2.0
0.135 < massDifference(0) < 0.155 on decay with \(\pi_{s}^{+}\) on \(D_{tag}^{*}\)
0.130 < massDifference(0) < 0.160 on decay with \(\pi^{0}\) on \(D_{tag}^{*}\)
0.120 < massDifference(0) < 0.165 on decay with \(\gamma\) on \(D_{tag}^{*}\)
1.81 < M < 2.21 on signal side \(D^{*+}\)
0.08 < \(M_{D^{*}}\) - \(M_{D}\) < 0.27 and p* > 2.0 on signal side \(D^{0}\)

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToHpHmHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to K- pi+ pi- pi+.
Skim name: DstToD0Pi_D0ToHpHmHpJm
Skim LFN code: 17241100
Category: physics, charm
Author: Kavita Lalwani, Chanchal Sharma
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \pi^+ \pi^- \pi^+ \pi^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \pi^+ \pi^- \pi^+ K^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \pi^+ \pi^- K^+ K^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \pi^+ K^- K^+ K^-\)

Selection Criteria:

Tracks from \(D^{0}\): abs(dr) < 1, abs(dz) < 3, thetaInCDCAcceptance
1.66 < M(D0) < 2.06
No cut on the slow pion
Q < 0.022, pcms(D*+) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Same as XToD0_D0ToHpJm, but requiring the D0 is from D*+ -> D0 pi+ process.
Skim name: DstToD0Pi_D0ToHpJm
Skim LFN code: 17240100
Category: physics, charm
Author: Giulia Casarosa
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to D^{0} \pi^+\), where \(D^{0}\) is reconstructed by XToD0_D0ToHpJm.D0ToHpJm

Selection Criteria:

Apply the cuts in XToD0_D0ToHpJm
No cut on the slow pion
0 < Q < 0.018
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToHpJmEta(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to pi+ D0, D0 to eta and two charged FSPs, where the kinds of two charged FSPs are different. The wrong-sign (WS) mode, D0 to K+ pi- eta, is also included.
Skim name: DstToD0Pi_D0ToHpJmEta
Skim LFN code: 17240500
Category: physics, charm
Author: Jaeyoung Kim
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to \pi^- D^{0}, D^{0}\to \pi^+ \pi^- \eta, \eta\to \gamma \gamma\)
\(RS: D^{*+}\to \pi^+ D^{0}, D^{0}\to K^- \pi^+ \eta, \eta\to \gamma \gamma\)
\(WS: D^{*+}\to \pi^+ D^{0}, D^{0}\to K^+ \pi^- \eta, \eta\to \gamma \gamma\)
\(D^{*+}\to \pi^- D^{0}, D^{0}\to K^+ K^- \eta, \eta\to \gamma \gamma\)

Selection Criteria:

Use tracks from the charm lists in charm_skim_std_charged
0.47 < M(eta) < 0.60, p(eta) > 0.24
1.66 < M(D0) < 2.06, pcms(D0) > 2.0
No cut on the slow pion
M(D*)-M(D0) < 0.16
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToHpJmKs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to pi+ D0, D0 to Ks and two conjugate charged FSPs.
Skim name: DstToD0Pi_D0ToHpJmKs
Skim LFN code: 17240700
Category: physics, charm
Author: Yeqi Chen
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}, D^{0}\to K_{S} \pi^+ \pi^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to K_{S} \pi^+ K^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to K_{S} K^+ \pi^-\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to K_{S} K^+ K^-\)

Selection Criteria:

Tracks from \(D^{0}\): abs(dr) < 1, abs(dz) < 3, thetaInCDCAcceptance
Use \(K_{S}\) from stdV0s.stdKshorts
1.66 < M(D0) < 2.06
No cut on the slow pion
Q < 0.022
pcms(D*) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToHpJmPi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*-tagged D0 to pi0 and two charged hadrons (any combination of kaons and pions).
Skim name: DstToD0Pi_D0ToHpJmPi0
Skim LFN code: 17240200
Category: physics, charm
Authors: Ludovico Massaccesi, Emma Oxford
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes: \(D^{*\pm}\to D^{0} \pi^\pm\) with

\(D^{0}\to K^\mp \pi^\pm \pi^0\) (and CC)
\(D^{0}\to \pi^+ \pi^- \pi^0\) (and CC)
\(D^{0}\to K^+ K^- \pi^0\) (and CC)

Selection Criteria:

Tracks: charmSkim lists from charm_skim_std_charged
- Pions: pionID > 0.1
- Kaons: kaonID > 0.1
\(\pi^{0}\): from stdPi0s.loadStdSkimPi0
1.70 < M(D0) < 2.10
M(D*)-M(D0) < 0.16
pCM(D*) > 2.0

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToKsOmega(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to pi+ D0, D0 to Ks pi+ pi- pi0.
Skim name: DstToD0Pi_D0ToKsOmega
Skim LFN code: 17240400
Category: physics, charm
Author: (no authors listed)
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}, D^{0}\to K_{S} \pi^+ \pi^- \pi^{0}\)

Selection Criteria:

Tracks from \(D^{0}\): abs(dr) < 1, abs(dz) < 3, thetaInCDCAcceptance
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0, then require 0.11 < M(pi0) < 0.15, p(pi0) > 0.25
1.66 < M(D0) < 2.06, pcms(D0) > 2.0
Q < 0.018
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToNeutrals(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Same as XToD0_D0ToNeutrals, but requiring that the D0 is from D* decay.
Skim name: DstToD0Pi_D0ToNeutrals
Skim LFN code: 17240600
Category: physics, charm
Authors: Giulia Casarosa, Emma Oxford
Contact: Jaeyoung Kim

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}\), where the \(D^{0}\) is reconstructed by XToD0_D0ToNeutrals.D0ToNeutrals.

Selection Criteria:

Apply the cuts in XToD0_D0ToNeutrals
No cut on the slow pion
deltaM<0.2
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToRare(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to pi+ D0, D0 to rare decay.
Skim name: DstToD0Pi_D0ToRare
Skim LFN code: 17230300
Category: physics, charm
Authors: Jaeyoung Kim, Doris Yangsoo Kim, Jaeyeon Kim
Contact: Jaeyoung Kim

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \gamma \gamma\),
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to ee\),
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to e^+ \mu^-\),
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to e^- \mu^+\),
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \mu \mu\),
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \pi^+ \pi^-\),

Selection Criteria:

Use photons from stdPhotons.loadStdSkimPhoton
Use electrons, muons, and pions from the charm_skim_std_charged
1.66 < M(D0) < 2.06
No cut on the slow pion
0 < Q < 0.02
pcms(D*) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToD0Pi_D0ToVGamma(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: A select of DstToD0Pi_D0ToVGamma, V is the vector meson, including phi, rho0, anti-K*0 and omega.
Skim name: DstToD0Pi_D0ToVGamma
Skim LFN code: 17241200
Category: physics, charm
Author: Jaeyoung Kim
Contact: Jaeyoung Kim

Decay Modes:

\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \phi \gamma\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \rho^{0} \gamma\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \bar K^{*0} \gamma\)
\(D^{*+}\to \pi^+ D^{0}, D^{0}\to \omega \gamma\)

Selection Criteria:

Use tracks from the charm lists in charm_skim_std_charged
Use \(\gamma\) from stdPhotons.loadStdSkimPhoton
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
Cut on \(\phi\): abs(dM) < 0.03
Cut on \(\rho^{0}\): abs(dM) < 0.3675
Cut on \(\bar K^{*0}\): abs(dM) < 0.33
Cut on \(\omega\): abs(dM) < 0.045
Cut on \(D^{0}\): abs(dM) < 0.225 and useCMSFrame(p) > 2
Cut on \(D^{*+}\): massDifference(0) < 0.160
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.DstToDpPi0_DpToHpPi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D*+ to D+ pi0, D+ to h+ pi0.
Skim name: DstToDpPi0_DpToHpPi0
Skim LFN code: 17241000
Category: physics, charm
Author: Johannes Brand
Contact: Jaeyoung Kim

Decay Modes:

\(D^{*+}\to \pi^{0} D^{+}, D^+ \to \pi^+ \pi^0\)

Selection Criteria:

Tracks: abs(dr) < 1, abs(dz) < 3, thetaInCDCAcceptance
Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
1.67 < M(D+) < 2.07, pcms(D+) > 2.0
0 < Q < 0.018
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.EarlyData_DstToD0Pi_D0ToHpHmPi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: A special version of DstToD0Pi_D0ToHpHmPi0 to deal with Early Data.
Skim name: EarlyData_DstToD0Pi_D0ToHpHmPi0
Skim LFN code: 17240900
Category: physics, charm
Author: (no authors listed)
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Cut criteria are not finally decided, and could be changed. Please check the code in the master branch to get up-to-date information.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.EarlyData_DstToD0Pi_D0ToHpJmPi0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: An special version of DstToD0Pi_D0ToHpJmPi0 to deal with Early Data.
Skim name: EarlyData_DstToD0Pi_D0ToHpJmPi0
Skim LFN code: 17240800
Category: physics, charm
Author: (no authors listed)
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Cut criteria are not finally decided, and could be changed. Please check the code in the master branch to get up-to-date information.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.LambdacToGeneric(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for inclusive Lambda_c+ decays.
Skim name: LambdacToGeneric
Skim LFN code: 17241400
Category: physics, charm
Author: Lukas Bierwirth
Contact: Jaeyoung Kim

Decay Modes:

Inclusive \(\Lambda_{c}^{+}\) is identified in mass recoiling against \(D^{(*)-} \bar{p} \pi^{+}\), \(D_{s}^{(*)-} \bar{p} K^{+}\), and \(D^{(*)0} \bar{p}\).
The tag side \(D\) is reconstructed in the following decay modes:
\(D^{*+}\to D^0 \pi^{+}\) and \(D^{*+}\to D^{+} \pi^{0}\) (tag side)
\(D^{*0}\to D^0 \pi^{0}\) and \(D^{*0}\to D^{0} \gamma\) (tag side)
\(D_s^{*+}\to D_s^{+} \gamma\) (tag side)
6 hadronic channels for tag \(D^{0}\) reconstruction
6 hadronic channels for tag \(D^{+}\) reconstruction
5 hadronic channels for tag \(D_{s}^{+}\) reconstruction

Selection Criteria:

Cut on \(\pi^{+}\) : abs(dr) < 0.5 and abs(dz) < 2.0
Cut on \(K^{+}\) : abs(dr) < 0.5 and abs(dz) < 2.0 and kaonID > 0.2
Cut on \(p\) : abs(dr) < 0.5 and abs(dz) < 2.0 and protonID > 0.2
Cut on \(\gamma\) : E > 0.10
Cut on \(\pi^{0}\to \gamma \gamma\): pi0:skim
Cut on tag side \(D^{0}\) : channel dependent mass window wider than \(3 \sigma\) and \(p^{*} > 1.8\)
Cut on tag side \(D^{+}\) : channel dependent mass window wider than \(3 \sigma\) and \(p^{*} > 1.8\)
Cut on tag side \(D_{s}^{+}\) : channel dependent mass window wider than \(3 \sigma\) and \(p^{*} > 1.8\)
0.120 < massDifference(0) < 0.176 on decay with \(\pi_{s}^{+}\) on \(D_{tag}^{*}\)
0.114 < massDifference(0) < 0.176 on decay with \(\pi^{0}\) on \(D_{tag}^{*}\)
0.104 < massDifference(0) < 0.190 on decay with \(\gamma\) on \(D_{tag}^{*}\)
1.4 < M < 3.4 and \(p^{*} > 1.8\) on signal side \(\Lambda_{c}^{+}\)
For more details, please check the source code of this skim.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.LambdacToSHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for Lambda_c+ three body decays including a Sigma+.
Skim name: LambdacToSHpJm
Skim LFN code: 17230900
Category: physics, charm
Author: Suravinda Kospalage
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(\Lambda_c^+ \to \Sigma^+ \pi^+ \pi^-\)
\(\Lambda_c^+ \to \Sigma^+ \pi^+ K^-\)
\(\Lambda_c^+ \to \Sigma^+ K^+ \pi^-\)
\(\Lambda_c^+ \to \Sigma^+ K^+ K^-\)
\(\Lambda_c^+ \to \Sigma^+ K_S\)

Selection Criteria:

Use tracks from the charm_skim_std_charged
2.2 < M(Lambda_c) < 2.4, pcms(Lambda_c) > 2.0
K/pi binary ID > 0.2, p/K/pi trinary ID > 0.2
loose mass window for \(\pi^{0}\) and skim selections from stdPi0s
0.44 < M(K_s) < 0.55, significanceOfFlightDistance > 2.0
\(\pm 3\sigma\) mass windows for \(\Sigma^+\)
lower bound on significance of distance for \(\Sigma^+\) > 2
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.LambdacTopHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for Lambda_c+ three body decays including a proton.
Skim name: LambdacTopHpJm
Skim LFN code: 17230600
Category: physics, charm
Author: Suravinda Kospalage
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(\Lambda_c^+ \to p \pi^+ \pi^-\)
\(\Lambda_c^+ \to p \pi^+ K^-\)
\(\Lambda_c^+ \to p K^+ \pi^-\)
\(\Lambda_c^+ \to p K^+ K^-\)

Selection Criteria:

Use tracks from the charm_skim_std_charged
2.2 < M(Lambda_c) < 2.4, pcms(Lambda_c) > 2.0
K/pi binary ID > 0.2, p/K/pi trinary ID > 0.2
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.XToD0_D0ToHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for inclusive D0 two body decays.
Skim name: XToD0_D0ToHpJm
Skim LFN code: 17230100
Category: physics, charm
Author: Dinura Hettiarachchi
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Skims \(D^0\)’s reconstructed by XToD0_D0ToHpJm.D0ToHpJm.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

static D0ToHpJm(path)[source]#

Decay Modes:

\(D^{0} \to \pi^+ \pi^-\),
\(D^{0} \to K^+ \pi^-\),
\(D^{0} \to K^- \pi^+\),
\(D^{0} \to K^+ K^-\),

Selection Criteria:

Use tracks from the charm_skim_std_charged
1.70 < M(D0) < 2.00, pcms(D0) > 2.0
`` K/pi binary ID > 0.2``
For more details, please check the source code of this skim.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#: Builds \(D^0\) skim lists defined in XToD0_D0ToHpJm.D0ToHpJm.

load_standard_lists(path)[source]#

class skim.WGs.charm.XToD0_D0ToNeutrals(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D0 to neutral FSPs.
Skim name: XToD0_D0ToNeutrals
Skim LFN code: 17230200
Category: physics, charm
Author: Giulia Casarosa
Contact: Jaeyoung Kim

Skims \(D^0\)’s reconstructed by XToD0_D0ToNeutrals.D0ToNeutrals.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

static D0ToNeutrals(path)[source]#

Decay Modes:

\(D^{0}\to \pi^{0} \pi^{0}\)
\(D^{0}\to K_{S} \pi^{0}\)
\(D^{0}\to K_{S} K_{S}\)

Selection Criteria:

Use \(\pi^{0}\) from stdPi0s.loadStdSkimPi0
Use \(K_{S}\) from stdV0s.stdKshorts
1.62 < M(D0) < 2.1, pcms(D0) > 2.0
For more details, please check the source code of this skim.
(Maybe in the future, we can add a loose ECL cluster timing cut to \(\pi^{0}\) in this skim.)

Parameters:

path (basf2.Path): Skim path to be processed.

Returns:

List of D0 particle list names.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#: Builds \(D^0\) skim lists defined in XToD0_D0ToNeutrals.D0ToNeutrals.

load_standard_lists(path)[source]#

class skim.WGs.charm.XToDp_DpToHpHmJp(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D_(s)+ to h+ h- j+.
Skim name: XToDp_DpToHpHmJp
Skim LFN code: 17230500
Category: physics, charm
Authors: Jaeyoung Kim, Aman Sangal
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^+_{(S)} \to \pi^+ \pi^- \pi^+\),
\(D^+_{(S)} \to \pi^+ \pi^- K^+\),
\(D^+_{(S)} \to \pi^+ K^- K^+\),
\(D^+_{(S)} \to K^+ K^- K^+\),
For \(D^+_{(S)} \to K_{S} h^+\), which includes a \(K_{S}\) vertex, please check XToDp_DpToKsHp

Selection Criteria:

Use traacks from the charm_skim_std_charged
Additional cut: global PID > 0.5(Temporary solution for Run1 re-skimming campaign. It might need to be modified.)
1.67 < M(D+) < 2.17, pcms(D+) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.XToDp_DpToKsHp(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for D_(s)+ to Ks h+.
Skim name: XToDp_DpToKsHp
Skim LFN code: 17230400
Category: physics, charm
Author: Guanda Gong
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(D^+_{(S)} \to K_{S} \pi^+\),
\(D^+_{(S)} \to K_{S} K^+\),

Selection Criteria:

Tracks not from \(K_{S}\): abs(dr) < 1, abs(dz) < 3, thetaInCDCAcceptance
Use \(K_{S}\) from stdV0s.stdKshorts and require flightDistance/flightDistanceErr > 2
1.67 < M(D+) < 2.17, pcms(D+) > 2.0
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.Xic0ToLHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for three-body Xi_c0 decays including a Lambda0
Skim name: Xic0ToLHpJm
Skim LFN code: 17231200
Category: physics, charm, cascade
Author: Saroj Pokharel
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(\Xi_c^0 \to \Lambda^0 \pi^+ K^-\)
\(\Xi_c^0 \to \Lambda^0 \pi^+ \pi^-\)
\(\Xi_c^0 \to \Lambda^0 K^+ K^-\)

Selection Criteria:

Use tracks from the charm_skim_std_charged
2.3 < M(Xi_c) < 2.65, pcms(Xi_c) > 2.0
p/K/pi trinary ID
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.XicToXimPipPim(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for Xi_c+ to hyperons.
Skim name: XicToXimPipPim
Skim LFN code: 17231100
Category: physics, charm, cascade
Author: Paul Gebeline
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes

\(\Xi_c^+ \to \Sigma^+ \pi^+ K^-\)
\(\Xi_c^+ \to \Sigma^+ K^+ K^-\)
\(\Xi_c^+ \to \Sigma^+ \pi^+ \pi^-\)
\(\Xi_c^+ \to \Xi^- \pi^+ \pi^-\)
\(\Xi_c^+ \to \Xi^0 \pi^+ \pi^+ \pi^-\)

Selection Criteria

standard track quality constraints on final state particles from charm_skim_std_charged
K/pi binary ID > 0.2, p/K/pi trinary ID > 0.2
\(\pm 3\sigma\) mass windows for all intermediate hyperons
\(\pm 3\sigma\) mass window for pi0 and skim selections from stdPi0s
lower bound on significance of (flight) distance for all intermediate hyperons, 40% of expected value to be used in analysis
loose mass window and lower bound to pCMS for Xic+
lower bound to p for pi0s originating from a Sigma+

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.XicpToLKsHp(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for Xi_c+ decaying to Lambda Ks h+, Xi- pi+ h+, Omega- pi+ K+.
Skim name: XicpToLKsHp
Skim LFN code: 17231300
Category: physics, charm, Xi_c
Author: Longke Li
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(\Xi_c^+ \to Lambda K_S^0 \pi^+\)
\(\Xi_c^+ \to Lambda K_S^0 K^+\)
\(\Xi_c^+ \to \Xi^- \pi^+ \pi^+\)
\(\Xi_c^+ \to \Xi^- \pi^+ K^+\)
\(\Xi_c^+ \to \Omega^- \pi^+ K^+\)

Selection Criteria:

Use tracks from the charm_skim_std_charged
2.35 < M(Xi_c) < 2.59, pcms(Xi_c) > 2.0

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.charm.XicpTopHpJm(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for Xi_c+ three body decays including a proton.
Skim name: XicpTopHpJm
Skim LFN code: 17231000
Category: physics, charm, cascade
Author: Suravinda Kospalage
Contact: Jaeyoung Kim

This skim includes a selection on the HLT flag hlt_hadron.

Decay Modes:

\(\Xi_c^+ \to p \pi^+ K^-\)

Selection Criteria:

Use tracks from the charm_skim_std_charged
2.3 < M(Xi_c) < 2.65, pcms(Xi_c) > 2.0
K/pi binary ID > 0.2, p/K/pi trinary ID > 0.2
For more details, please check the source code of this skim.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['ParticleLoader', 'RootOutput']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

skim.WGs.charm.charm_skim_sigma(path)[source]#: Provides a list of charged sigma baryons for charm skims with these basic cuts applied: 1.166 < M < 1.211 and significanceOfDistance > 2. The proton daughters must fulfil a loose proton PID requirement vs pions and kaons and the pi0 daughters are standard skim pi0s with an invariant mass in the range 0.12 - 0.145 GeV/c^2.

skim.WGs.charm.charm_skim_std_charged(particle_type, path)[source]#: Provides a list of charged particles to be used by charm skims named <particle_type>+:charmSkim, with basic cuts applied: dr < 1 and abs(dz) < 3 and thetaInCDCAcceptance.

21.2.4. Dark sector skims#

Skim list building functions for the dark sector physics working group

class skim.WGs.dark.AA2uuuu(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: \(ee\to A^{\prime}A^{\prime}\nu_{D}\nu_{D}\to \mu\mu\mu\mu\)
Skim name: AA2uuuu
Skim LFN code: 18370100
Category: physics, dark sector
Author: Chanyoung LEE
Contact: Gaurav Sharma

Searching dark photons in 4-muon final state.

Reconstructed a muon pair to a dark photon.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.ALP3Gamma(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Neutral dark sector skim list for the ALP 3-photon analysis: \(ee\to a(\to\gamma\gamma)\gamma\)
Skim name: ALP3Gamma
Skim LFN code: 18020300
Category: physics, dark sector
Author: Michael De Nuccio
Contact: Gaurav Sharma

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

addALPToPDG()[source]#: Adds the ALP codes to the basf2 pdg instance

additional_setup(path)[source]#

build_lists(path)[source]#

initialALP(path)[source]#

An list builder function for the ALP decays. Part of the ALP3Gamma skim.

Parameters:: path (basf2.Path) – the path to add the skim
Returns:: list name of the ALP decays candidates

class skim.WGs.dark.BtoK_ALP2Gamma(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Dark-sector skim selecting \(B \to K^{(*)}a(\to \gamma \gamma)\) candidates by reconstructing A0->gamma gamma, K*->Kpi resonances, and B meson decay chains.
Skim name: BtoK_ALP2Gamma
Skim LFN code: 18020800
Category: physics, dark sector
Author: Hyuna Kim
Contact: Gaurav Sharma

Physics channel: \(B \to K^{(*)}a(\to \gamma \gamma)\)

Cuts applied: * Kaons:BtoK_ALP2Gamma -> kaonID > 0.1, dr < 3.0, abs(dz) < 4.0 * Pions:BtoK_ALP2Gamma-> pionID > 0.1, dr < 3.0, abs(dz) < 4.0 * Photons:BtoK_ALP2Gamma-> E > 0.05 * A0 candidate: daughter(0,E) > daughter(1,E) * K*0/K*+: 0.8 < M < 1.0 * B candidates: Mbc > 5.20, abs(deltaE) < 1.0

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.BtoKplusLLP(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: B+ to K+ LLP analysis skim \(e^{+}e^{-} \to \Upsilon(4s) \to [B^{+} \to K^{+} LLP]B^{-}\)
Skim name: BtoKplusLLP
Skim LFN code: 18130100
Category: physics, dark sector
Author: Sascha Dreyer
Contact: Gaurav Sharma

Skim to select B+ decays to a K+ from the IP and a LLP with a vertex displaced from the IR decaying to two charged tracks.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DarkShower(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for the dark shower analysis. We are reconstructing the displaced vertex as a \(e^+e^- \to K_s(\to \pi^+ \pi^-)\)
Skim name: DarkShower
Skim LFN code: 18022500
Category: physics, dark sector
Author: Miho Wakai
Contact: Gaurav Sharma

Skim list contains events with only one displaced vertex and a maximum of one other good track.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DielectronPlusMissingEnergy(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Dielectron skim, needed for \(e^{+}e^{-} \to A^{\prime} h^{\prime};\)\(A^{\prime} \to e^{+}e^{-}; \, h^{\prime} \to \mathrm{invisible}\) and other searches.
Skim name: DielectronPlusMissingEnergy
Skim LFN code: 18520300
Category: physics, dark sector
Author: Giacomo De Pietro
Contact: Gaurav Sharma

Physics channel: \(e^{+}e^{-} \to e^{+}e^{-}\)

Warning

This skim is currently deactivated, since the retention rate is too high.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'mumu'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DielectronPlusVisibleDarkHiggs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for the visible dark higgs analysis
Skim name: DielectronPlusVisibleDarkHiggs
Skim LFN code: 18020700
Category: physics, dark sector
Author: Luigi Corona
Contact: Gaurav Sharma

Physics channel: e+e- -> A’h’, A’-> e+e-, hp -> tr+tr-

Skim list contains candidates for the visible dark Higgs produced in association with a prompt electron-pair.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

addParticlesToPDG()[source]#: Adds the particle codes to the basf2 pdg instance

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DimuonPlusMissingEnergy(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Dimuon + missing energy skim, needed for \(e^{+}e^{-} \to \mu^{+}\mu^{-}Z^{\prime}; \, Z^{\prime} \to \mathrm{invisible}\) and other searches.
Skim name: DimuonPlusMissingEnergy
Skim LFN code: 18520100
Category: physics, dark sector
Author: Giacomo De Pietro
Contact: Gaurav Sharma

Physics channel: \(e^{+}e^{-} \to \mu^{+}\mu^{-} \, +\) missing energy.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DimuonPlusVisibleDarkHiggs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for the visible dark higgs analysis
Skim name: DimuonPlusVisibleDarkHiggs
Skim LFN code: 18020600
Category: physics, dark sector
Author: Luigi Corona
Contact: Gaurav Sharma

Physics channel: e+e- -> A’h’, A’-> mu+mu-, hp -> tr+tr-

Skim list contains candidates for the visible dark Higgs produced in association with a a prompt muon-pair.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

addParticlesToPDG()[source]#: Adds the particle codes to the basf2 pdg instance

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.DimuonRecoilMassSquared(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Dimuon skim, needed for \(e^{+}e^{-} \to A^{\prime} \to \mu^{+}\mu^{-} (\gamma)\) and other searches.
Skim name: DimuonRecoilMassSquared
Skim LFN code: 18022400
Category: physics, dark sector
Author: Robin Leboucher
Contact: Gaurav Sharma

Physics channel: \(e^{+}e^{-} \to \mu^{+}\mu^{-} \gamma\).

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.EGammaControlDark(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Electron-gamma skim list for study of the ee backgrounds at high dark photon mass, as part of the dark photon analysis
Skim name: EGammaControlDark
Skim LFN code: 18020400
Category: physics, dark sector, control-channel
Authors: Sam Cunliffe, Torben Ferber
Contact: Gaurav Sharma

Physics channel: ee → eγ

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.ElectronMuonPlusMissingEnergy(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Electron-muon pair + missing energy skim, needed for \(e^{+}e^{-} \to e^{\pm}\mu^{\mp} Z^{\prime}; \, Z^{\prime} \to \mathrm{invisible}\) and other searches.
Skim name: ElectronMuonPlusMissingEnergy
Skim LFN code: 18520200
Category: physics, dark sector
Author: Giacomo De Pietro
Contact: Gaurav Sharma

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#: Physics channel: \(e^{+}e^{-} \to e^{\pm}\mu^{\mp} \, +\) missing energy

load_standard_lists(path)[source]#

class skim.WGs.dark.GammaGammaControlKLMDark(prescale_high=1, prescale_low=1, **kwargs)[source]#

Note

Skim description: Gamma gamma skim list for study of the KLM efficiency as part of the dark photon analysis
Skim name: GammaGammaControlKLMDark
Skim LFN code: 18020200
Category: physics, dark sector, control-channel
Authors: Sam Cunliffe, Miho Wakai
Contact: Gaurav Sharma

Physics channel: ee → γγ

Note

This skim can retain a lot of γγ events. In case this becomes unacceptable, we provide prescale parameters. Prescales are given in standard trigger convention (reciprocal), so prescale of 100 is 1% of events kept, etc.

Tip

To prescale the higher-energy probe photons by 10%:

>>> from skim.WGs.dark import GammaGammaControlKLMDark
>>> Skim = GammaGammaControlKLMDark(prescale_high=10)
>>> Skim(path)  # Add list-building function and uDST output module to path
>>> b2.process(path)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'gg'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.InelasticDarkMatter(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: iDM list for the iDM analysis.
Skim name: InelasticDarkMatter
Skim LFN code: 18000000
Category: physics, dark sector
Author: Savino Longo
Contact: Gaurav Sharma

Skim list contains events with no tracks from IP, no high E tracks and only one high E photon.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.InelasticDarkMatterWithDarkHiggs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for the inelastic Dark Matter with a Dark Higgs analysis.
Skim name: InelasticDarkMatterWithDarkHiggs
Skim LFN code: 18020500
Category: physics, dark sector
Author: Patrick Ecker
Contact: Gaurav Sharma

Skim list contains events with at least one displaced vertex and no additional unused tracks from the IP.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

addParticlesToPDG()[source]#: Adds the particle codes to the basf2 pdg instance

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.LFVZpVisible(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Lepton flavour violating Z’ skim, Z’ to visible FS.
Skim name: LFVZpVisible
Skim LFN code: 18520400
Category: physics, dark sector
Author: Ilya Komarov and Luigi Corona
Contact: Gaurav Sharma

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#: Physics channel: ee –> e mu Z’; Z’ –> e mu

load_standard_lists(path)[source]#

class skim.WGs.dark.RadBhabhaV0Control(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: iDM control sample skim. \(e^{+}e^{-} \to e^{+}e^{-}V^{0};\)
Skim name: RadBhabhaV0Control
Skim LFN code: 18000001
Category: physics, dark sector
Author: Savino Longo
Contact: Gaurav Sharma

Control sample: \(e^{+}e^{-} \to e^{+}e^{-}V^{0};\)”

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.SinglePhotonDark(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Single photon skim list for the dark photon analysis.
Skim name: SinglePhotonDark
Skim LFN code: 18020100
Category: physics, dark sector
Authors: Sam Cunliffe, Chris Hearty
Contact: Gaurav Sharma

Physics channel: ee → A’γ; A’ → invisible

Skim list contains single photon candidates for the dark photon to invisible final state analysis.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.dark.TopologicalDarkPion(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Single pi0 skim, needed for \(e^{+}e^{-} \to \gamma \to \pi^{0}\chi_{1} \chi_{2}\) and other searches.
Skim name: TopologicalDarkPion
Skim LFN code: 18020900
Category: physics, dark sector
Author: Guorui Liu
Contact: Gaurav Sharma

Physics channel: \(e^{+}e^{-} \to \pi^{0}\chi_{1} \chi_{2}\)

Decay Modes: \(\pi^{0}\to \gamma \gamma\)

Cuts applied:

2 std_all photon with thetaInCDCAcceptance and E > 0.04 GeV and -200 ns < clusterTiming < 200 ns
pi0 0.09 GeV/c^2 < InvM < 1 GeV/c^2
daughters opening angle in CMS frame < 80 degrees
daughter highest E and highest Ecms > 0.7 GeV
0 < nParticlesInList(pi0) < 4
no track [abs(dz) < 2 cm and pt > 0.3 GeV/c] or [abs(dz) < 2 cm and p > 0.4GeV/c]
no extra photon Ecms > 1 GeV
total energy of pi0 daughters in CMS frame < 7 GeV

Note

This skim uses skim.standardlists.charm.loadStdD0_Kpipi0, where the \(\overline{D}{}^{0}\) channel is defined.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

21.2.5. Full event interpretation skims#

(Semi-)Leptonic Working Group Skims for missing energy modes that use the Full event interpretation (FEI) algorithm.

class skim.WGs.fei.BaseFEISkim(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Base class for FEI skims. Applies event-level pre-cuts and applies the FEI.

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

FEIChannelArgs = {}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

FEIPrefix = 'FEIv1_2025_MC16ri_aldebaran_200'#: Prefix label for the FEI training used in the FEI skims.

MergeDataStructures = {'FEIChannelArgs': <function _merge_boolean_dicts>}#: Dict of str -> function pairs to determine if any special data structures should be merged when combining skims. Currently, this is only used to merge FEI config parameters when running multiple FEI skims at once, so that it can be run just once with all the necessary arguments.

NoisyModules = ['ParticleCombiner']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

additional_setup(path)[source]#

Apply pre-FEI event-level cuts and apply the FEI. This setup function is run by all FEI skims, so they all have the same event-level pre-cuts.

This function passes FEIChannelArgs to the cached function run_fei_for_skims to avoid applying the FEI twice.

See also

fei_precuts for event-level cut definitions.

static fei_precuts(path)[source]#

Skim pre-cuts are applied before running the FEI, to reduce computation time. This setup function is run by all FEI skims, so they all have the save event-level pre-cuts:

\(n_{\text{cleaned tracks}} \geq 3\)
\(n_{\text{cleaned ECL clusters}} \geq 3\)
\(\text{Visible energy of event (CMS frame)}>4~{\rm GeV}\)

We define “cleaned” tracks and clusters as:

Cleaned tracks (pi+:FEI_cleaned): \(d_0 < 0.5~{\rm cm}\), \(|z_0| < 2~{\rm cm}\), and \(p_T > 0.1~{\rm GeV}\)
Cleaned ECL clusters (gamma:FEI_cleaned): \(\theta\) in CDC acceptance, and \(E>0.1~{\rm GeV}\)

produce_on_tau_samples = True#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

static run_fei_for_skims(FEIChannelArgs, FEIPrefix, analysisGlobaltag, *, path)[source]#

Reconstruct hadronic and semileptonic \(B^0\) and \(B^+\) tags using the generically trained FEI.

Parameters:

FEIChannelArgs (dict(str, bool)) – A dict of keyword-boolean pairs to be passed to fei.get_default_channels.
FEIPrefix (str) – Prefix label for the FEI training used in the FEI skims.
path (basf2.Path) – The skim path to be processed.

static setup_fei_aliases(FEIChannelArgs)[source]#

class skim.WGs.fei.feiHadronic(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged neutral and charged \(B\)’s decaying hadronically.
Skim name: feiHadronic
Skim LFN code: 11180500
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(M_{\text{bc}} > 5.2~{\rm GeV}\)
\(|\Delta E| < 0.3~{\rm GeV}\)
\(\text{signal probability} > 0.001\) (omitted for decay mode 25 for \(B^+\), and decay mode 23 for \(B^0\))

All available FEI \(B^0\) and \(B^+\) hadronic tags are reconstructed. From Thomas Keck’s thesis, “the channel \(B^0 \to \overline{D}^0 \pi^0\) was used by the FR, but is not yet used in the FEI due to unexpected technical restrictions in the KFitter algorithm”.

List of reconstructed channels and corresponding decay mode IDs:

B0 channels:

\(B^0_{\text{had}} \to D^- \pi^+\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to \overline{D}^0 \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- D^0 K^+\)
\(B^0_{\text{had}} \to D^- D^{0*} K^+\)
\(B^0_{\text{had}} \to D^{-*} D^0 K^+\)
\(B^0_{\text{had}} \to D^{-*} D^{0*} K^+\)
\(B^0_{\text{had}} \to D^- D^+ K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^+ K^0_S\)
\(B^0_{\text{had}} \to D^- D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^+_s D^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to D^{+*}_s D^-\)
\(B^0_{\text{had}} \to D^+_s D^{-*}\)
\(B^0_{\text{had}} \to D^{+*}_s D^{-*}\)
\(B^0_{\text{had}} \to J/\psi K^0_S\)
\(B^0_{\text{had}} \to J/\psi K^+ \pi^-\)
\(B^0_{\text{had}} \to J/\psi K^0_S \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p}\)
\(B^0_{\text{had}} \to D^- p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+ \pi^-\)

B+ channels:

\(B^+_{\text{had}} \to \overline{D}^0 \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{0*} K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{0*} K^+\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to D^{+*}_s \overline{D}^0\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^{0*}\)
\(B^+_{\text{had}} \to \overline{D}^0 K^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^+\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^0_S \pi^+\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^- \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to D^+ p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to D^{+*} p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': True, 'hadronic': True, 'neutralB': True, 'semileptonic': False}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

class skim.WGs.fei.feiHadronicB0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged neutral \(B\)’s decaying hadronically.
Skim name: feiHadronicB0
Skim LFN code: 11180100
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(M_{\text{bc}} > 5.2~{\rm GeV}\)
\(|\Delta E| < 0.3~{\rm GeV}\)
\(\text{signal probability} > 0.001\) (omitted for decay mode 23)

All available FEI \(B^0\) hadronic tags are reconstructed. From Thomas Keck’s thesis, “the channel \(B^0 \to \overline{D}^0 \pi^0\) was used by the FR, but is not yet used in the FEI due to unexpected technical restrictions in the KFitter algorithm”.

List of reconstructed channels and corresponding decay mode IDs:

\(B^0_{\text{had}} \to D^- \pi^+\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to \overline{D}^0 \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- D^0 K^+\)
\(B^0_{\text{had}} \to D^- D^{0*} K^+\)
\(B^0_{\text{had}} \to D^{-*} D^0 K^+\)
\(B^0_{\text{had}} \to D^{-*} D^{0*} K^+\)
\(B^0_{\text{had}} \to D^- D^+ K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^+ K^0_S\)
\(B^0_{\text{had}} \to D^- D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^+_s D^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to D^{+*}_s D^-\)
\(B^0_{\text{had}} \to D^+_s D^{-*}\)
\(B^0_{\text{had}} \to D^{+*}_s D^{-*}\)
\(B^0_{\text{had}} \to J/\psi K^0_S\)
\(B^0_{\text{had}} \to J/\psi K^+ \pi^-\)
\(B^0_{\text{had}} \to J/\psi K^0_S \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p}\)
\(B^0_{\text{had}} \to D^- p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+ \pi^-\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': False, 'hadronic': True, 'neutralB': True, 'semileptonic': False}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.fei.feiHadronicBplus(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged charged \(B\)’s decaying hadronically.
Skim name: feiHadronicBplus
Skim LFN code: 11180200
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(M_{\text{bc}} > 5.2~{\rm GeV}\)
\(|\Delta E| < 0.3~{\rm GeV}\)
\(\text{signal probability} > 0.001\) (omitted for decay mode 25)

All available FEI \(B^+\) hadronic tags are reconstructed.

List of reconstructed channels and corresponding decay mode IDs:

\(B^+_{\text{had}} \to \overline{D}^0 \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{0*} K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{0*} K^+\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to D^{+*}_s \overline{D}^0\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^{0*}\)
\(B^+_{\text{had}} \to \overline{D}^0 K^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^+\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^0_S \pi^+\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^- \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to D^+ p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to D^{+*} p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': True, 'hadronic': True, 'neutralB': False, 'semileptonic': False}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.fei.feiHadronic_DstEllNu(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged neutral and charged \(B\)’s decaying hadronically. Analysis specific cuts applied during skimming. Best 2 candidates ranked by sigProb kept
Skim name: feiHadronic_DstEllNu
Skim LFN code: 11180501
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(M_{\text{bc}} > 5.27~{\rm GeV}\)
\(-0.150 < \Delta E < 0.100~{\rm GeV}\)
\(\text{signal probability} > 0.001\) (omitted for decay mode 25 for \(B^+\), and decay mode 23 for \(B^0\))
\(\cos{TBTO} < 0.9\)
Selects only the two best candidates that survive based on the signalProbability

All available FEI \(B^0\) and \(B^+\) hadronic tags are reconstructed. From Thomas Keck’s thesis, “the channel \(B^0 \to \overline{D}^0 \pi^0\) was used by the FR, but is not yet used in the FEI due to unexpected technical restrictions in the KFitter algorithm”.

List of reconstructed channels and corresponding decay mode IDs:

B0 channels:

\(B^0_{\text{had}} \to D^- \pi^+\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to \overline{D}^0 \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^- D^0 K^+\)
\(B^0_{\text{had}} \to D^- D^{0*} K^+\)
\(B^0_{\text{had}} \to D^{-*} D^0 K^+\)
\(B^0_{\text{had}} \to D^{-*} D^{0*} K^+\)
\(B^0_{\text{had}} \to D^- D^+ K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^+ K^0_S\)
\(B^0_{\text{had}} \to D^- D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^{-*} D^{+*} K^0_S\)
\(B^0_{\text{had}} \to D^+_s D^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^0 \pi^0\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^-\)
\(B^0_{\text{had}} \to D^{-*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^0_{\text{had}} \to D^{+*}_s D^-\)
\(B^0_{\text{had}} \to D^+_s D^{-*}\)
\(B^0_{\text{had}} \to D^{+*}_s D^{-*}\)
\(B^0_{\text{had}} \to J/\psi K^0_S\)
\(B^0_{\text{had}} \to J/\psi K^+ \pi^-\)
\(B^0_{\text{had}} \to J/\psi K^0_S \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p}\)
\(B^0_{\text{had}} \to D^- p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to D^{-*} p \bar{p} \pi^+\)
\(B^0_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+ \pi^-\)
\(B^0_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+ \pi^-\)

B+ channels:

\(B^+_{\text{had}} \to \overline{D}^0 \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^0 \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^+ K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{+*} K^0_S\)
\(B^+_{\text{had}} \to \overline{D}^0 D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^0 K^+\)
\(B^+_{\text{had}} \to \overline{D}^0 D^{0*} K^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} D^{0*} K^+\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^0 \pi^0\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \overline{D}^{0*} \pi^+ \pi^+ \pi^- \pi^0\)
\(B^+_{\text{had}} \to D^{+*}_s \overline{D}^0\)
\(B^+_{\text{had}} \to D^+_s \overline{D}^{0*}\)
\(B^+_{\text{had}} \to \overline{D}^0 K^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+\)
\(B^+_{\text{had}} \to D^- \pi^+ \pi^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^+\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^+ \pi^-\)
\(B^+_{\text{had}} \to J/\psi K^+ \pi^0\)
\(B^+_{\text{had}} \to J/\psi K^0_S \pi^+\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^0\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+ \pi^- \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^0 p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to \overline{D}^{0*} p \bar{p} \pi^+\)
\(B^+_{\text{had}} \to D^+ p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to D^{+*} p \bar{p} \pi^+ \pi^-\)
\(B^+_{\text{had}} \to \Lambda^{-}_{c} p \pi^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': True, 'hadronic': True, 'neutralB': True, 'semileptonic': False}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

class skim.WGs.fei.feiSL(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged neutral and charged \(B\)’s decaying semileptonically.
Skim name: feiSL
Skim LFN code: 11180600
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(-4 < \cos\theta_{BY} < 3\)
\(\log_{10}(\text{signal probability}) > -2.4\)
\(p_{\ell}^{*} > 1.0~{\rm GeV}\) in CMS frame

SL \(B^0\) and \(B^+\) tags are reconstructed. Hadronic \(B\) with SL \(D\) are not reconstructed, as these are rare and time-intensive.

List of reconstructed channels and corresponding decay mode IDs:

B0 channels:

\(B^0_{\text{SL}} \to D^- e^+\)
\(B^0_{\text{SL}} \to D^- \mu^+\)
\(B^0_{\text{SL}} \to D^{-*} e^+\)
\(B^0_{\text{SL}} \to D^{-*} \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- \mu^+\)

B+ channels:

\(B^+_{\text{SL}} \to \overline{D}^0 e^+\)
\(B^+_{\text{SL}} \to \overline{D}^0 \mu^+\)
\(B^+_{\text{SL}} \to \overline{D}^{0*} e^+\)
\(B^+_{\text{SL}} \to \overline{D}^{0*} \mu^+\)
\(B^+_{\text{SL}} \to D^- \pi^+ e^+\)
\(B^+_{\text{SL}} \to D^- \pi^+ \mu^+\)
\(B^+_{\text{SL}} \to D^{-*} \pi^+ e^+\)
\(B^+_{\text{SL}} \to D^{-*} \pi^+ \mu^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': True, 'hadronic': False, 'neutralB': True, 'removeSLD': True, 'semileptonic': True}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

class skim.WGs.fei.feiSLB0(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged neutral \(B\)’s decaying semileptonically.
Skim name: feiSLB0
Skim LFN code: 11180300
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(-4 < \cos\theta_{BY} < 3\)
\(\log_{10}(\text{signal probability}) > -2.4\)
\(p_{\ell}^{*} > 1.0~{\rm GeV}\) in CMS frame

SL \(B^0\) tags are reconstructed. Hadronic \(B\) with SL \(D\) are not reconstructed, as these are rare and time-intensive.

List of reconstructed channels and corresponding decay mode IDs:

\(B^0_{\text{SL}} \to D^- e^+\)
\(B^0_{\text{SL}} \to D^- \mu^+\)
\(B^0_{\text{SL}} \to D^{-*} e^+\)
\(B^0_{\text{SL}} \to D^{-*} \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- \mu^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': False, 'hadronic': False, 'neutralB': True, 'removeSLD': True, 'semileptonic': True}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.fei.feiSLB0_RDstar(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (“FEI-tagged neutral \(B\)’s decaying semileptonically”, ‘Analysis cuts included, best sigProb candidate kept’)
Skim name: feiSLB0_RDstar
Skim LFN code: 11180301
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(\text{FoxWolframR2} < 0.4\)
\(-1.75 < \cos\theta_{BY} < 1.1\)
\(\log_{10}(\text{signal probability}) > -2.0\)
\(p_{\ell}^{*} > 1.0~{\rm GeV}\) in CMS frame
\(\text{BCS:signal probability}\)

SL \(B^0\) tags are reconstructed. Hadronic \(B\) with SL \(D\) are not reconstructed, as these are rare and time-intensive.

List of reconstructed channels and corresponding decay mode IDs:

\(B^0_{\text{SL}} \to D^- e^+\)
\(B^0_{\text{SL}} \to D^- \mu^+\)
\(B^0_{\text{SL}} \to D^{-*} e^+\)
\(B^0_{\text{SL}} \to D^{-*} \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^0 \pi^- \mu^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- e^+\)
\(B^0_{\text{SL}} \to \overline{D}^{0*} \pi^- \mu^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': False, 'hadronic': False, 'neutralB': True, 'removeSLD': True, 'semileptonic': True}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.fei.feiSLBplus(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: FEI-tagged charged \(B\)’s decaying semileptonically.
Skim name: feiSLBplus
Skim LFN code: 11180400
Category: physics, Full Event Interpretation
Authors: Racha Cheaib, Hannah Wakeling, Phil Grace
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Tag side \(B\) cuts:

\(-4 < \cos\theta_{BY} < 3\)
\(\log_{10}(\text{signal probability}) > -2.4\)
\(p_{\ell}^{*} > 1.0~{\rm GeV}\) in CMS frame

SL \(B^+\) tags are reconstructed. Hadronic \(B^+\) with SL \(D\) are not reconstructed, as these are rare and time-intensive.

List of reconstructed channels and corresponding decay mode IDs:

\(B^+_{\text{SL}} \to \overline{D}^0 e^+\)
\(B^+_{\text{SL}} \to \overline{D}^0 \mu^+\)
\(B^+_{\text{SL}} \to \overline{D}^{0*} e^+\)
\(B^+_{\text{SL}} \to \overline{D}^{0*} \mu^+\)
\(B^+_{\text{SL}} \to D^- \pi^+ e^+\)
\(B^+_{\text{SL}} \to D^- \pi^+ \mu^+\)
\(B^+_{\text{SL}} \to D^{-*} \pi^+ e^+\)
\(B^+_{\text{SL}} \to D^{-*} \pi^+ \mu^+\)

See also

BaseFEISkim.FEIPrefix for FEI training used, and BaseFEISkim.fei_precuts for event-level cuts made before applying the FEI.

FEIChannelArgs = {'KLong': False, 'baryonic': True, 'chargedB': True, 'hadronic': False, 'neutralB': False, 'removeSLD': True, 'semileptonic': True}#: Dict of str -> bool pairs to be passed to fei.get_default_channels. When inheriting from BaseFEISkim, override this value to apply the FEI for only e.g. SL charged \(B\)’s.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

21.2.6. Leptonic skims#

(Semi-)Leptonic Working Group Skims for leptonic analyses.

class skim.WGs.leptonic.LeptonicUntagged(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for leptonic analyses, \(B_{\text{sig}}^-\to\ell\nu\), where \(\ell=e,\mu\)
Skim name: LeptonicUntagged
Skim LFN code: 11130300
Category: physics, leptonic
Author: Daniel Jacobi
Contacts: Cameron Harris, Tommy Martinov

Reconstructed decays

\(B^- \to e^-\)
\(B^- \to \mu^-\)

Cuts applied

\(p_{\ell}^{*} > 1.8\,\text{GeV}\) in CMS Frame
\(\text{electronID} > 0.5\)
\(\text{muonID} > 0.5\)
\(n_{\text{tracks}} \geq 3\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

21.2.7. Low multiplicity skims#

Skim list building functions for the low multiplicity physics working group

class skim.WGs.lowMulti.LowMassOneTrack(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for low mass events with one track and one hard photon in final state.
Skim name: LowMassOneTrack
Skim LFN code: 18530600
Category: physics, low multiplicity
Authors: Gaurav Sharma, Qingyuan Liu
Contact: Gaurav Sharma

Physics channel: \(e^{+}e^{-} \to \gamma \pi^{+}\pi^{-}\) and \(e^{+}e^{-} \to \gamma \mu^{+}\mu^{-}\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'mumu'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

class skim.WGs.lowMulti.LowMassTwoTrack(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim list for low mass events with at least two tracks and one hard photon in final state.
Skim name: LowMassTwoTrack
Skim LFN code: 18520500
Category: physics, low multiplicity
Authors: Xing-Yu Zhou, Guanda Gong
Contact: Xing-Yu Zhou

Physics channel: \(e^{+}e^{-} \to \gamma h_{1}^{+}h_{2}^{-} X\)

Warning

This skim includes the golden mode \(e^{+}e^{-} \to \gamma \pi^{+}\pi^{-}\)

Note

The \(h_{1}^{+}\) and \(h_{2}^{+}\) here mean a positive particle and a negative particle that could be either conjugate or non-conjugate. The \(X\) means arbitrary final state particles.

Decay Modes

\(e^{+}e^{-} \to \gamma \pi^{+} \pi^{-} X\),
\(e^{+}e^{-} \to \gamma K^{+} K^{-} X\),
\(e^{+}e^{-} \to \gamma K^{+} \pi^{-} X\),
\(e^{+}e^{-} \to \gamma p \overline{p} X\),
\(e^{+}e^{-} \to \gamma p \pi^{-} X\),
\(e^{+}e^{-} \to \gamma p K^{-} X\),
\(e^{+}e^{-} \to \gamma \mu^{+} \mu^{-} X\),

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'mumu'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.lowMulti.SingleTagPseudoScalar(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: A skim script to select events with one high-energy electron and one or more pi0/eta/eta mesons.
Skim name: SingleTagPseudoScalar
Skim LFN code: 18530200
Category: physics, low multiplicity
Author: Hisaki Hayashii
Contact: Hisaki Hayashii

Physics channel: \(e^{+}e^{-} \to e^{\pm} (e^{\mp}) \pi^{0}/\eta/\eta^{\prime}\)

Decay Modes

\(\pi^{0}\to \gamma \gamma\),
\(\eta \to \gamma\gamma\),
\(\eta \to \pi^{+}\pi^{-}\pi^{0}\),
\(\eta \to \pi^{+}\pi^{-}\gamma\),
\(\eta^{\prime} \to \pi^{+}\pi^{-}\eta(\to \gamma\gamma)\),
\(\eta^{\prime} \to \pi^{+}\pi^{-}\gamma\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.lowMulti.TwoTrackLeptonsForLuminosity(prescale=1, **kwargs)[source]#

Note

Skim description: Skim list for two track lepton (e+e- to e+e- and e+e- to mu+mu-) events for luminosity measurements.
Skim name: TwoTrackLeptonsForLuminosity
Skim LFN code: 18530100
Category: physics, low multiplicity
Author: Xing-Yu Zhou
Contact: Xing-Yu Zhou

Physics channel: \(e^{+}e^{-} \to e^{+}e^{-}\) and \(e^{+}e^{-} \to \mu^{+}\mu^{-}\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'mumu'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

21.2.8. Quarkonium skims#

Skim list building functions for quarkonium analyses: bottomonium, charmonium, resonance

class skim.WGs.quarkonium.BottomoniumEtabExclusive(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BottomoniumEtabExclusive
Skim LFN code: 15420100
Category: physics, quarkonium
Authors: Stefano Spataro, Sen Jia
Contact: Sen Jia

Reconstructed decay modes:

eta_b -> gamma gamma

Selection criteria:

2 std photon with E > 3.5 GeV
7 < M(eta_b) < 10 GeV/c^2
foxWolframR2 < 0.995

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.quarkonium.BottomoniumUpsilon(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: BottomoniumUpsilon
Skim LFN code: 15440100
Category: physics, quarkonium
Authors: Stefano Spataro, Sen Jia
Contact: Sen Jia

Reconstructed decay modes:

Y(1S,2S) -> l^+ l^{-} (l = e or mu)

Selection criteria:

2 tracks with momentum ranging between 3.5 < p < 15
At least 1 track p < 1.5 or 1 std photon with E > 150 MeV
M(Y(1S,2S)) > 8 GeV/c^2
foxWolframR2 < 0.995

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.quarkonium.CharmoniumPsi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Selection of J/psi and psi(2S) via leptonic decays.
Skim name: CharmoniumPsi
Skim LFN code: 16460200
Category: physics, quarkonium
Author: Kirill Chilikin
Contact: Sen Jia

Reconstructed decay modes:

J/psi -> l^+ l^- (l = e or mu)
psi(2S) -> l^+ l^- (l = e or mu)

Selection criteria:

2 tracks with electronID > 0.1 or muonID > 0.1 and 2.85 < M < 3.9. Track-quality requirements are not applied.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.quarkonium.InclusiveLambda(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Inclusive Lambda skim
Skim name: InclusiveLambda
Skim LFN code: 15410300
Category: physics, quarkonium
Author: Bianca Scavino
Contact: Sen Jia

Reconstructed decay:

\(\Lambda \to p \pi^-\) (and charge conjugate)

Selection criteria:

Cuts on proton:

protonID > 0.1

Cuts on Lambda:

cosAngleBetweenMomentumAndVertexVector > 0.75
flightDistance/flightDistanceErr > 0.
0.5 < p_proton/p_Lambda < 1.25 GeV/c

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.quarkonium.InclusiveUpsilon(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Inclusive Upsilon(1S,2S,3S) skim
Skim name: InclusiveUpsilon
Skim LFN code: 15460400
Category: physics, quarkonium
Author: Sen Jia
Contact: Sen Jia

Reconstructed decay modes:

Upsilon(1S,2S,3S) -> l^+ l^- (l = e or mu)

Selection criteria:

3 charged tracks or 2 charged tracks + 1 std photon 8.5 < M < 10.6 for e+e- mode and M > 8.5 for mu+mu- mode

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

21.2.9. Radiative and electroweak penguins skims#

Skim list building functions for EWP inclusive skims: B->Xgamma, B->Xll, B->Xll (LFV modes)

class skim.WGs.ewp.B0TwoBody(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for 2 body B0 decays
Skim name: B0TwoBody
Skim LFN code: 12120400
Category: Physics, 2 Body, no PID
Author: Ryan Mueller and Santi Naylor
Contact: Ihor Prudiiev

Reconstructed decays

\(B^0 \to e^+ e^-\)
\(B^0 \to e^+ \mu^-\)
\(B^0 \to e^- \mu^+\)
\(B^0 \to \mu^+ \mu^-\)
\(B^0 \to \pi^+ \pi^-\)

Cuts applied

\(n_{\text{tracks}} \geq 3\)
\(|\delta E| < 0.5 \text{GeV}\)
\(M_{bc} > 5.2 \text{GeV}/c^2\)
\(dr < 0.5 \text{cm}, |dz| < 2 \text{cm}\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.ewp.BtoXgamma(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: \(B\to X\gamma\) inclusive skim.
Skim name: BtoXgamma
Skim LFN code: 12160100
Category: physics, electroweak penguins, radiative decays
Author: Trevor Shillington
Contact: Ihor Prudiiev

Reconstructed decay modes:

\(B^+ \to X\gamma\) inclusive

Event-level cuts:

\(\text{foxWolframR2} < 0.7\) constructed using tracks with \(p_T>0.1\,\text{GeV}\) and clusters with \(E>0.1\,\text{GeV}\).
\(n_{\text{tracks}} \geq 3\)

Cuts on photons:

\(\text{clusterE9E21}>0.9\)
\(1.4\,\text{GeV}< E_{\gamma}<3.4\,\text{GeV}\) in CMS frame

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#: Build the skim list for \(B \to X\gamma\) decays.

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.ewp.BtoXll(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: \(B\to X\ell\ell\) (no LFV modes) inclusive skim.
Skim name: BtoXll
Skim LFN code: 12160200
Category: physics, electroweak penguins, radiative decays
Author: Trevor Shillington
Contact: Ihor Prudiiev

Reconstructed decay modes:

\(B^+ \to X e^+ e^-\)
\(B^+ \to X e^+ e^+\)
\(B^+ \to X \mu^+ \mu^-\)
\(B^+ \to X \mu^+ \mu^+\)

Event-level cuts:

\(\text{foxWolframR2} < 0.7\) constructed using tracks with \(p_T>0.1\,\text{GeV}\) and clusters with \(E>0.1\,\text{GeV}\).
\(n_{\text{tracks}} \geq 3\)

Cuts on electrons:

\(\text{electronID} > 0.1\)
\(p > 0.395\,\text{GeV}\) in lab frame
\(dr<0.5\) and \(abs(dz)<2\)

Cuts on muons:

\(\text{muonID} > 0.5\)
\(p > 0.395\,\text{GeV}\) in lab frame
\(dr<0.5\) and \(abs(dz)<2\)

Cut on dilepton energy:

\(E_{\ell\ell}>1.5\,\text{GeV}\) in CMS frame.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#: Build the skim list for \(B \to X\ell\ell\) non-LFV decays.

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.ewp.BtoXll_LFV(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: \(B\to X\ell\ell\) (LFV modes only) inclusive skim.
Skim name: BtoXll_LFV
Skim LFN code: 12160300
Category: physics, electroweak penguins, radiative decays
Author: Trevor Shillington
Contact: Ihor Prudiiev

Reconstructed decay modes:

\(B^+ \to X e^+ \mu^-\)
\(B^+ \to X \mu^+ e^-\)
\(B^+ \to X e^+ \mu^+\)

Event-level cuts:

\(\text{foxWolframR2} < 0.7\) constructed using tracks with \(p_T>0.1\,\text{GeV}\) and clusters with \(E>0.1\,\text{GeV}\).
\(n_{\text{tracks}} \geq 3\)

Cuts on electrons:

\(\text{electronID} > 0.1\)
\(p > 0.395\,\text{GeV}\) in lab frame
\(dr<0.5\) and \(abs(dz)<2\)

Cuts on muons:

\(\text{muonID} > 0.5\)
\(p > 0.395\,\text{GeV}\) in lab frame
\(dr<0.5\) and \(abs(dz)<2\)

Cut on dilepton energy:

\(E_{\ell\ell}>1.5\,\text{GeV}\) in CMS frame.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#: Build the skim list for \(B \to X\ell\ell\) LFV decays.

load_standard_lists(path)[source]#

class skim.WGs.ewp.FourLepton(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for 4 body leptonic analyses
Skim name: FourLepton
Skim LFN code: 12120500
Category: Physics, Leptonic, 4 Body
Author: Santi Naylor and Ryan Mueller
Contact: Ihor Prudiiev

Reconstructed decays

\(B^0 \to e^- e^+ e^- e^+\)
\(B^0 \to e^- e^+ mu^- mu^+\)

Cuts applied

\(n_{\text{tracks}} \geq 5\)
\(-1.5 < \delta E < 0.5 \text{GeV}\)
\(5.2 < M_{bc} < 5.3 \text{GeV}/c^2\)
\(dr < 0.5 \text{cm}, |dz| < 2 \text{cm}\)
\(muonID>0.1\)
\(electronID>0.1\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.ewp.RadiativeDilepton(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for 3 body leptonic analyses
Skim name: RadiativeDilepton
Skim LFN code: 12120600
Category: Physics, Leptonic, 3 body
Author: Santi Naylor and Ryan Mueller
Contact: Ihor Prudiiev

Reconstructed decays

\(B^0 \to e^- e^+ \gamma\)
\(B^0 \to mu^- mu^+ \gamma\)

Cuts applied

\(n_{\text{tracks}} \geq 3\)
\(-1.0 < \delta E < 0.5 \text{GeV}\)
:math:` 5.2 < M_{bc} < 5.3 text{GeV}/c^2`
\(dr < 0.5 \text{cm}, |dz| < 2 \text{cm}\)
\(muonID>0.1\)
\(electronID>0.1\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

21.2.10. Semileptonic skims#

(Semi-)Leptonic Working Group Skim list building functions for semi-leptonic analyses.

class skim.WGs.semileptonic.B0toDstarl_Kpi_Kpipi0_Kpipipi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: (no description)
Skim name: B0toDstarl_Kpi_Kpipi0_Kpipipi
Skim LFN code: 11160201
Category: physics, semileptonic
Author: Bae Hanwook, Chiara La Licata
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Cuts applied:

SkimHighEff tracks thetaInCDCAcceptance AND dr < 2 AND abs(dz) < 5 AND PID>=0.01
slowPi tracks thetaInCDCAcceptance AND dr < 2 AND abs(dz) < 5 AND useCMSFrame(p) < 0.4
\(2.5 > p_{\ell} > 1.1\,\text{GeV}\)
lepton with abs(dr) < 0.5 AND abs(dz) < 2 AND thetaInCDCAcceptance AND ID >= 0.95 AND 1.1 < useCMSFrame(p) < 2.5
1.8 < M_D0 < 2.0
DM_Dstar_D < 0.16

Reconstructed decays:

\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^-) e^+\),
\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^- \pi^0) e^+\),
\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^- \pi^- \pi^+) e^+\),
\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^-) mu^+\),
\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^- \pi^0) mu^+\),
\(B^{0}\to D^{*-} (D^{0} \to K^+ \pi^- \pi^- \pi^+) mu^+\),

Note

This skim uses skim.standardlists.charm.loadSkimHighEffD0_Kpi, skim.standardlists.charm.loadSkimHighEffD0_Kpipipi and skim.standardlists.charm.loadStdD0_eff20_Kpipi0, where \(D^0\) channel is defined. skim.standardlists.charm.loadSkimHighEffDstarPlus_D0pi_Kpi, skim.standardlists.charm.loadSkimHighEffDstarPlus_D0pi_Kpipipi, skim.standardlists.charm.loadStdDstarPlus_D0pi_Kpipi0_eff20,where the \(D^{*-}\) channel is defined.

The pion and kaon lists used to define \(D^0\) and \(D^{*-}\) are: skim.standardlists.charm.loadPiSkimHighEff, skim.standardlists.charm.loadKSkimHighEff and skim.standardlists.charm.loadSlowPi

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

class skim.WGs.semileptonic.BtoDl_and_ROE_e_or_mu_or_lowmult(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for semileptonic tags with an ROE electron, muon, photon or a low-multiplicity signal decay
Skim name: BtoDl_and_ROE_e_or_mu_or_lowmult
Skim LFN code: 11170100
Category: physics, semileptonic
Author: Bob Kowalewski
Contacts: Cameron Harris, Tommy Martinov

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decay modes:

\(B^- \to D^0 e^-\), \(B^- \to D^0 \mu^-\)
anti-\(B^0 \to D^+ e^-\), anti-\(B^0 \to D^+ \mu^-\)
anti-\(B^0 \to D^{*+}(D^0 \pi^+) e^-\), anti-\(B^0 \to D^{*+}(D^0 \pi^+) \mu^-\)

Additional ROE cuts:

The logical OR of the following:
- identified \(e^{\pm}\) with \(p(CM) < 3.0\) GeV
- identified \(\mu^{\pm}\) with \(p(CM) < 3.0\) GeV
- identified \(\gamma\) with \(E(CM) > 1.4\) GeV
- Two or fewer charged tracks
- \(E_{ECL} < 2.0\) GeV

Cuts on electrons:

\(\text{electronID} > 0.3\)
\(p_t > 0.3\,\text{GeV}\) in lab frame, \(p > 0.5\,\text{GeV}\) in lab frame
\(dr < 0.5\), \(|dz| < 2\)
\(\text{thetaInCDCAcceptance}\)

Cuts on muons:

\(\text{muonID} > 0.9\)
\(p_t > 0.4\,\text{GeV}\) in lab frame, \(p > 0.7\,\text{GeV}\) in lab frame
\(dr < 0.5\), \(|dz| < 2\)

Charged mask for ROE:

\(p_t>0.05\,\text{GeV}\)
\(dr < 5\,\text{cm}\), \(|dz| < 10\,\text{cm}\)

ECL cluster mask for ROE:

\(\text{clusterNHits}>1.5\), \(\theta\) in CDC acceptance
\(E>0.080,\text{GeV}\)

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

TestSampleProcess = 'charged'#: MC process of test file. BaseSkim.TestFiles passes this property to skim.utils.testfiles.get_test_file to retrieve an appropriate file location. Defaults to a \(B^{0}\overline{B^{0}}\) sample.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.semileptonic.PRsemileptonicUntagged(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for partial reconstruction analysis in leptonic group.
Skim name: PRsemileptonicUntagged
Skim LFN code: 11110100
Category: physics, semileptonic
Authors: Lucien Cremaldi, Racha Cheaib, Romulus Godang
Contacts: Cameron Harris, Tommy Martinov

Reconstructed decay modes:

\(B^0 \to \pi^- e^+\)
\(B^0 \to \pi^- \mu^+\)

Event-level cuts:

\(\text{foxWolframR2} < 0.5\) constructed using tracks with \(p_T>0.1\,\text{GeV}\) and clusters with \(E>0.1\,\text{GeV}\).
\(n_{\text{tracks}} > 4\)

Cuts on electrons:

\(\text{electronID} > 0.5\)
\(p > 1.5\,\text{GeV}\) in CMS frame

Cuts on muons:

\(\text{muonID} > 0.5\)
\(p > 1.5\,\text{GeV}\) in CMS frame

Cuts on pions:

\(\text{pionID}>0.5\)
\(\text{muonID}<0.2\)
\(0.060\,\text{GeV}<p<0.220\,\text{GeV}\) in CMS frame

Cuts on partially reconstructed \(B\) mesons:

\(\cos\theta_{\ell,\,\pi}<0\) in CMS frame.

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.semileptonic.SLUntagged(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for semileptonic decays, \(B\) decays (\(B \to D \ell\nu\), where \(\ell=e,\mu\))
Skim name: SLUntagged
Skim LFN code: 11160200
Category: physics, semileptonic
Authors: Phillip Urquijo, Racha Cheaib
Contacts: Cameron Harris, Tommy Martinov

Cuts applied:

\(p_{\ell} > 0.35\,\text{GeV}\)
\(5.24 < M_{\text{bc}} < 5.29\)
\(|\Delta E | < 0.5\)
\(n_{\text{tracks}} > 4\)

Reconstructed decays:

\(B^+ \to \overline{D}^{0} e^+\)
\(B^+ \to \overline{D}^{0} \mu^+\)
\(B^+ \to \overline{D}^{*0} e^+\)
\(B^+ \to \overline{D}^{*0} \mu^+\)
\(B^0 \to D^{-} e^+\)
\(B^0 \to D^{-} \mu^+\)
\(B^0 \to D^{*-} e^+\)
\(B^0 \to D^{*-} \mu^+\)

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

21.2.11. Time-dependent CP-violation (TDCPV) analysis skims#

class skim.WGs.tdcpv.TDCPV_ccs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for time-dependent CP violation analysis.
Skim name: TDCPV_ccs
Skim LFN code: 13160200
Category: physics, TDCPV
Authors: Reem Rasheed, Chiara La Licata, Stefano Lacaprara
Contact: Noah BRENNY

This skim includes a selection on the HLT flag hlt_hadron.

Physics channels: bd → ccs

Decay Channels:

\(B^0 \to J/\psi (ee/\mu\mu) K_S^0\)
\(B^0 \to \psi(2S) (ee/\mu\mu) K_S^0\)
\(B^0 \to J/\psi (ee/\mu\mu) K^* (K^+ \pi^- / K_S^0 \pi^0)\)
\(B^+ \to J/\psi (ee/\mu\mu) K^+\)
\(B^0 \to J/\psi (ee/\mu\mu) K_L\)
\(B^0 \to J/\psi (ee/\mu\mu) \eta (\pi^+ \pi^- \pi^0 / \pi^+ \pi^-)\)
\(B^0 \to J/\psi (ee/\mu\mu) \pi^0\)
\(B^0 \to J/\psi (ee/\mu\mu) K^+ \pi^-\)
\(B^+ \to J/\psi (ee/\mu\mu) K^{*+} (\pi^+ K_S^0 / K^+ \pi^0)\)

Particle lists used:

K_S0:merged
pi+:all
J/psi:ee
J/psi:mumu
psi(2S):ee
psi(2S):mumu
K*0:SkimHighEff
K+:SkimHighEff
K_L0:allklm
K_L0:allecl
eta:SkimHighEff
pi0:eff40_May2020
pi0:eff60_May2020

Cuts used:

SkimHighEff tracks thetaInCDCAcceptance AND chiProb > 0 AND abs(dr) < 0.5 AND abs(dz) < 3 and PID>0.01
5.2 < Mbc < 5.29 for Ks/K*
abs(deltaE) < 0.3 and 5.05 < Mbc < 5.29 for KL
abs(deltaE) < 0.5
nCleanedTracks(abs(dz) < 2.0 and abs(dr) < 0.5 and nCDCHits>20)>=3
nCleanedECLClusters(thetaInCDCAcceptance and E>0.2)>1
visibleEnergyOfEventCMS>4
E_ECL_TDCPV < 9

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.tdcpv.TDCPV_dilepton(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Inclusive dilepton skim
Skim name: TDCPV_dilepton
Skim LFN code: 13130300
Category: physics, leptonic
Author: Alessandro Gaz, Chiara La Licata
Contact: Noah BRENNY

This skim includes a selection on the HLT flag hlt_hadron.

Reconstructed decays

\(B\overline{B} \to l^+l^-\)
\(B\overline{B} \to l^+l^+\)
\(B\overline{B} \to l^-l^-\)

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

NoisyModules = ['EventShapeCalculator']#: List of module types to be silenced. This may be necessary in certain skims in order to keep log file sizes small.

Tip

The elements of this list should be the module type, which is not necessarily the same as the module name. The module type can be inspected in Python via module.type().

See also

This attribute is used by BaseSkim.set_skim_logging.

build_lists(path)[source]#

load_standard_lists(path)[source]#

class skim.WGs.tdcpv.TDCPV_inclusiveJpsi(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Inclusive J/psi (ee/mumu) skim for time-dependent CP violation analysis.
Skim name: TDCPV_inclusiveJpsi
Skim LFN code: 13110100
Category: physics, TDCPV
Authors: Xu Dong, Thibaud Humair, Tadeas Bilka
Contact: Noah BRENNY

This skim includes a selection on the HLT flag hlt_hadron.

Physics channels: bd → ccs

This skims inclusive J/psi events, which include Psi(2S) to dileptons as well as Psi(2S) to J/psi X or chi_c1 to J/psi gamma

Decay Channels:

\(B^0 \to J/\psi (ee/\mu\mu) X\)

Cuts used:

abs(d0) < 0.5 and abs(z0) < 2.0 and thetaInCDCAcceptance for muon and electron tracks
muonID_noSVD > 0.01 for muons and electronID > 0.01 for electrons as PID cuts
E < 1 for photons for Bremsstrahlung correction for electrons
2.7 < M < 4.1 and useCMSFrame(p) < 3.1 for J/psi (or Psi(2S)) reconstruction

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.tdcpv.TDCPV_klong(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for time-dependent CP violation analysis b->qqs decays using Klongs
Skim name: TDCPV_klong
Skim LFN code: 13160400
Category: physics, TDCPV
Authors: Michele Veronesi, Noah Brenny
Contact: Noah BRENNY

This skim includes a selection on the HLT flag hlt_hadron.

Physics channels: bd/u → qqs with Klongs

Decay Channels:

\(B^0 \to \phi K_L^0\)
\(B^0 \to \eta ' K_L^0\)
\(B^0 \to \omega K_L^0\)
\(B^0 \to \rho^0 K_L^0\)
\(B^0 \to \pi^0 K_L^0\)

Particle lists used:

phi:SkimHighEff
eta:SkimHighEff1
eta:SkimHighEff2
rho0:SkimHighEff
K_L0:allklm
K_L0:allecl

Cuts used:

SkimHighEff tracks thetaInCDCAcceptance AND chiProb > 0 AND abs(dr) < 0.5 AND abs(dz) < 3 and PID>0.01
clusterE>0.150 for loose ECL KL
klmClusterInnermostLayer<=10 and klmClusterLayers<=10 for loose KLM KL
clusterPulseShapeDiscriminationMVA<0.15 and clusterE>0.25 for tight ECL KL
klmClusterKlId>0.1 and klmClusterInnermostLayer<=10 and klmClusterLayers<=10 for tight KLM KL
abs(deltaE) < 0.1
nCleanedECLClusters(thetaInCDCAcceptance and E>0.2)>1,
E_ECL_TDCPV < 9
foxWolframR2<0.6

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.tdcpv.TDCPV_qqs(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for time-dependent CP violation analysis b->qqs decays
Skim name: TDCPV_qqs
Skim LFN code: 13160300
Category: physics, TDCPV
Authors: Reem Rasheed, Chiara La Licata, Stefano Lacaprara
Contact: Noah BRENNY

This skim includes a selection on the HLT flag hlt_hadron.

Physics channels: bd/u → qqs

Decay Channels:

\(B^0 \to \phi K_S^0\)
\(B^0 \to \phi K^{*0}\)
\(B^0 \to \eta K_S^0\)
\(B^0 \to \eta' K_S^0\)
\(B^0 \to \eta K^{*0}\)
\(B^0 \to \eta' K^{*0}\)
\(B^0 \to K_S^0 K_S^0 K_S^0\)
\(B^0 \to \pi^0 K_S^0\)
\(B^0 \to \rho^0 K_S^0\)
\(B^0 \to \omega K_S^0\)
\(B^0 \to f_0 K_S^0\)
\(B^0 \to \pi^0 \pi^0 K_S^0\)
\(B^0 \to \phi K_S^0 \pi^0\)
\(B^0 \to \pi^+ \pi^- K_S^0\)
\(B^0 \to \pi^+ \pi^- K_S^0 \gamma\)
\(B^0 \to \pi^0 K_S^0 \gamma\)
\(B^0 \to \phi K_S^0 \gamma\)
\(B^0 \to \eta K_S^0 \gamma\)
\(B^0 \to \rho^0 \gamma\)
\(B^0 \to \omega \gamma\)
\(B^0 \to \phi \gamma\)
\(B^+ \to \eta' K^+\)
\(B^+ \to \phi K^+\)
\(B^+ \to \phi K^{*+}\)
\(B^+ \to \omega K^+\)
\(B^+ \to \rho^0 K^+\)
\(B^+ \to K_S^0 K_S^0 K^+\)
\(B^+ \to \pi^+ \pi^- K^+ \gamma\)

Particle lists used:

phi:SkimHighEff
eta':SkimHighEff
eta:SkimHighEff
pi0:eff40_May2020
pi0:skim
pi0:SkimHighEff
rho0:SkimHighEff
omega:SkimHighEff
f_0:SkimHighEff
pi+:SkimHighEff
K+:SkimHighEff
omega:SkimHighEff
K*0:SkimHighEff
gamma:E15 , cut : 1.4 < E < 4
gamma:ECMS16 , cut : 1.6 < useCMSFrame(E)
K_S0:merged
K+:1%

Cuts used:

SkimHighEff tracks thetaInCDCAcceptance AND chiProb > 0 AND abs(dr) < 0.5 AND abs(dz) < 3 and PID>0.01
5.2 < Mbc < 5.29
abs(deltaE) < 0.5
nCleanedECLClusters(thetaInCDCAcceptance and E>0.2)>1
E_ECL_TDCPV < 9

ApplyHLTHadronCut = True#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

build_lists(path)[source]#

load_standard_lists(path)[source]#

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

21.2.12. Tau-pair skims#

Skim list building functions for tau-pair analyses

class skim.WGs.taupair.TauGeneric(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for Tau generic decays.
Skim name: TauGeneric
Skim LFN code: 18570600
Category: physics, tau
Author: Kenji Inami
Contact: Kenji Inami

Channel: \(e^+ e^- \to \tau^+ \tau^-\)

Criteria:

Ntrk = 2

Number of good tracks = 2, net charge < 2
visibleEnergyOfEventCMS < 10 GeV and E_ECLtrk < 6 GeV and missingMomentumOfEvent_theta < 2.6180
visibleEnergyOfEventCMS > 3 GeV or max P_t > 1 GeV
max. opening angle < 178 deg.

Ntrk = 3,4

Number of good tracks = 3 or 4, net charge < 2
visibleEnergyOfEventCMS < 10.5 GeV and E_ECLtrk < 6 GeV
visibleEnergyOfEventCMS > 3 GeV or max P_t > 1 GeV
max. opening angle < 178 deg.
Event divided by thrust axis; No. good tracks in tag side = 1 or 3
M_tag < 1.8 GeV and M_sig < 2.3 GeV

Ntrk = 5,6

Number of good tracks = 5 or 6, net charge < 2
Event divided by thrust axis; No. good tracks in tag side = 1 or 3
M_tag < 1.8 GeV and M_sig < 2.3 GeV

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

Set particle lists and variables for TauGeneric skim.

Output particle lists: * pi+:tauskim, pi0:tauskim, gamma:pi0_tauskim, gamma:nonpi0_tauskim, gamma:tauskim, pi+:S1/S2, pi0:S1/S2, gamma:S1/S2

Variables:

nGoodTracks: number of good tracks in an event
netCharge: total net charge of good tracks
nTracksS1/nTracksS2: number of good tracks in each hemisphere S1/S2 divided by thrust axis
invMS1/invMS2: invariant mass of particles in each hemisphere
maxPt: maximum Pt among good tracks
E_ECLtrk: total ECL energy of good tracks

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.taupair.TauKshort(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for Tau decays with Kshort.
Skim name: TauKshort
Skim LFN code: 18570800
Category: physics, tau
Authors: Paolo Leo, Kenji Inami
Contact: Kenji Inami

Channel: \(e^+ e^- \to \tau^+ \tau^-, \tau \to K_s \pi X\)

Criteria:

nAlltracks < 7
0.9 < thrust < 0.995
2.5 < visibleEnergyOfEventCMS < 10 GeV
0.2 < track_kshort_pt < 4.5
max(kshort_track1_pt,kshort_track2_pt) > 0.25
track_kshort_significanceOfDistance > 3

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

Set particle lists and variables for TauKshort skim.

Constructed particle lists: * pi+:tauKs, pi0:tauKs, gamma:pi0_tauKs, gamma:nonpi0_tauKs, gamma:tauKs, pi+:tauKsS1/tauKsS2

Variables:

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.taupair.TauLFV(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for Tau LFV decays.
Skim name: TauLFV
Skim LFN code: 18360100
Category: physics, tau
Author: Kenji Inami
Contact: Kenji Inami

Channel: \(\tau \to l \gamma, lll, l \pi^0, l \eta, l \eta', l K_S, l f_0, l V^0, lhh, llp, phh, \lambda\pi\)

Output particle lists: e+:taulfv, mu+:taulfv, pi+:taulfv, K+:taulfv, p+:taulfv, gamma:taulfv, pi0:taulfv, K_S0:taulfv, eta:taulfv, eta':taulfv, omega:taulfv, Lambda0:taulfv_p, Lambda0:taulfv_antip

Criteria for 1 prong final states: Number of good tracks < 5, \(1.0 < M < 2.0\) GeV, \(-1.5 < \Delta E < 0.5\) GeV

Criteria for >1 prong final states: Number of good tracks < 7, \(1.4 < M < 2.0\) GeV, \(-1.0 < \Delta E < 0.5\) GeV

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

class skim.WGs.taupair.TauThrust(*, OutputFileName=None, additionalDataDescription=None, udstOutput=True, validation=False, mc=True, analysisGlobaltag=None, pidGlobaltag=None)[source]#

Note

Skim description: Skim for Tau decays using thrust.
Skim name: TauThrust
Skim LFN code: 18570700
Category: physics, tau
Authors: Ami Rostomyan, Kenji Inami
Contact: Kenji Inami

Channel: \(e^+ e^- \to \tau^+ \tau^-\)

Criteria:

1 < No. good tracks < 7
net charge == 0
Event divided by thrust axis; select 1x1, 1x3, 1x5, 3x3 topology
0.8 < thrust
visibleEnergyOfEventCMS < 10.4 GeV
For 1x1 topology, thrust < 0.99
For 1x1 topology, 1.5 < visibleEnergyOfEventCMS

ApplyHLTHadronCut = False#: If this property is set to True, then the HLT selection for hlt_hadron will be applied to the skim lists when the skim is added to the path.

additional_setup(path)[source]#

Set particle lists and variables for TauThrust skim.

Constructed particle lists: * pi+:thrust, pi0:thust, gamma:pi0_thrust, gamma:nonpi0_thrust, gamma:thrust, pi+:thrustS1/thrustS2

Variables:

nGoodTracksThrust: number of good tracks in an event
netChargeThrust: total net charge of good tracks
nTracksS1Thrust/nTracksS2Thrust: number of good tracks in each hemisphere S1/S2 divided by thrust axis

build_lists(path)[source]#

load_standard_lists(path)[source]#

produce_on_tau_samples = False#

If this property is set to False, then b2skim-prod will not produce data production requests for this skim on taupair MC samples. This decision may be made for one of two reasons:

The retention rate of the skim on taupair samples is basically zero, so there is no point producing the skim for these samples.
The retention rate of the skim on taupair samples is too high (>20%), so the production system may struggle to handle the jobs.

validation_histograms(path)[source]#

validation_sample = 'mdst16.root'#: MDST sample to use for validation histograms. Must be a valid location of a validation dataset (see documentation for basf2.find_file).

skim.WGs.taupair.tauskim_particle_selection(label, path)[source]#

Physics skims

Contents

21.2. Physics skims#

21.2.1. B → charm skims#

21.2.2. B → charmless skims#

21.2.3. Charm physics skims#

21.2.4. Dark sector skims#

21.2.5. Full event interpretation skims#

21.2.6. Leptonic skims#

21.2.7. Low multiplicity skims#

21.2.8. Quarkonium skims#

21.2.9. Radiative and electroweak penguins skims#

21.2.10. Semileptonic skims#

21.2.11. Time-dependent CP-violation (TDCPV) analysis skims#

21.2.12. Tau-pair skims#