caf_ecl_time_crate.py

 
"""ECL timing calibration that performs the crate calibrations, one for each physics run."""
 
from prompt import CalibrationSettings
from reconstruction import prepare_cdst_analysis
 

 

settings = CalibrationSettings(
    name="ECL crate time calibrations",
    expert_username="ehill",
    description=__doc__,
    input_data_formats=["cdst"],
    input_data_names=["bhabha_combined_calib"],
    # input_data_filters={
    #     "bhabha_combined_calib": [
    #         input_data_filters["Data Tag"]["bhabha_combined_calib"],
    #         input_data_filters["Beam Energy"]["4S"],
    #         input_data_filters["Beam Energy"]["Continuum"],
    #         input_data_filters["Beam Energy"]["Scan"],
    #         input_data_filters["Data Quality Tag"]["Good"],
    #         input_data_filters["Run Type"]["physics"],
    #         input_data_filters["Magnet"]["On"],
    #     ]
    # },
    depends_on=[],
)
 
 

 

 
 
def get_calibrations(input_data, **kwargs):
    """
    Parameters:
      input_data (dict): Should contain every name from the 'input_data_names' variable as a key.
        Each value is a dictionary with {"/path/to/file_e1_r5.root": IoV(1,5,1,5), ...}. Useful for
        assigning to calibration.files_to_iov
 
      **kwargs: Configuration options to be sent in. Since this may change we use kwargs as a way to help prevent
        backwards compatibility problems. But you could use the correct arguments in b2caf-prompt-run for this
        release explicitly if you want to.
 
        Currently only kwargs["output_iov"] is used. This is the output IoV range that your payloads should
        correspond to. Generally your highest ExpRun payload should be open ended e.g. IoV(3,4,-1,-1)
 
    Returns:
      list(caf.framework.Calibration): All of the calibration objects we want to assign to the CAF process
    """
    import basf2
    # Set up config options
 
    # In this script we want to use one sources of input data.
    # Get the input files  from the input_data variable
    # The input data should be the bhabha skim
    file_to_iov_physics = input_data["bhabha_combined_calib"]
 
    # We might have requested an enormous amount of data across a run range.
    # There's a LOT more files than runs!
    # Lets set some limits because this calibration doesn't need that much to run.
    max_files_per_run = 26
 
    # We filter addition files if there are more than [max_files_per_run] files per run.
    # The input data files are sorted alphabetically by b2caf-prompt-run
    # already. This procedure respects that ordering
    from prompt.utils import filter_by_max_files_per_run
 
    reduced_file_to_iov_physics = filter_by_max_files_per_run(
        file_to_iov_physics, max_files_per_run
    )
    input_files_physics = list(reduced_file_to_iov_physics.keys())
    basf2.B2INFO(
        f"Total number of files actually used as input = {len(input_files_physics)}"
    )
 
    
    from basf2 import register_module, create_path
    from ROOT import Belle2
    from caf.framework import Collection
 
    
    root_input = register_module("RootInput")
    rec_path_bhabha = create_path()
    rec_path_bhabha.add_module(root_input)
    if "Gearbox" not in rec_path_bhabha:
        rec_path_bhabha.add_module("Gearbox")
    if "Geometry" not in rec_path_bhabha:
        rec_path_bhabha.add_module("Geometry", useDB=True)
 
    prepare_cdst_analysis(rec_path_bhabha)  # for new 2020 cdst format
 
    # ====================================================
    t0BiasCorrection = -0.9  # Correct for the CDC t0 bias
    # ====================================================
 
    col_bhabha = register_module("ECLBhabhaTCollector")
    col_bhabha.param("timeAbsMax", 250)
    col_bhabha.param("minCrystal", 1)
    col_bhabha.param("maxCrystal", 8736)
    col_bhabha.param("saveTree", False)
    col_bhabha.param("hadronEventT0_TO_bhabhaEventT0_correction", t0BiasCorrection)
 
    eclTCol = Collection(
        collector=col_bhabha,
        input_files=input_files_physics,
        pre_collector_path=rec_path_bhabha,
    )
 
    
 
    eclTAlg = Belle2.ECL.eclBhabhaTAlgorithm()
 
    # Define the CAF algorithm arguments
    # Set the cellIDLo to be larger than cellIDHi so that no crystal
    #    calibrations will be performed.
    eclTAlg.cellIDLo = 3
    eclTAlg.cellIDHi = 2
    eclTAlg.debugOutput = True
    eclTAlg.meanCleanRebinFactor = 3
    eclTAlg.meanCleanCutMinFactor = 0.3
    eclTAlg.debugFilenameBase = "eclBhabhaTAlgorithm"
 
    
 
    from caf.framework import Calibration
 
    cal_test = Calibration("ECLcrateTimeCalibration_physics")
    cal_test.add_collection(name="bhabha", collection=eclTCol)
    cal_test.algorithms = [eclTAlg]
 
    # Here we set the AlgorithmStrategy for our algorithm
    from caf.strategies import SimpleRunByRun
 
    # The SimpleRunByRun strategy executes your algorithm over runs
    # individually to give you payloads for each one (if successful)
    # It will not do any merging of runs which didn't contain enough data.
    # So failure is expected if your algorithm requires a large amount of data compared to run length.
    # You should only use granularity='run' for the collector when using this strategy.
 
    cal_test.strategies = SimpleRunByRun
 
    # Most other options like database chain and backend args will be overwritten by b2caf-prompt-run.
    # So we don't bother setting them.
 
    # You must return all calibrations you want to run in the prompt process, even if it's only one
    return [cal_test]