BeamParametersFitter.cc

/**************************************************************************
 * basf2 (Belle II Analysis Software Framework)                           *
 * Author: The Belle II Collaboration                                     *
 *                                                                        *
 * See git log for contributors and copyright holders.                    *
 * This file is licensed under LGPL-3.0, see LICENSE.md.                  *
 **************************************************************************/
 
/* Own header. */
#include <reconstruction/calibration/BeamSpotBoostInvMass/BeamParametersFitter.h>
 
/* Basf2 headers. */
#include <framework/database/Database.h>
#include <framework/database/DBImportObjPtr.h>
#include <framework/database/DBStore.h>
#include <framework/gearbox/Const.h>
#include <framework/logging/Logger.h>
 
/* ROOT headers. */
#include <TMinuit.h>
#include <TVectorD.h>
#include <Math/Vector3D.h>
#include <Math/Vector4D.h>
#include <Math/VectorUtil.h>
#include <Math/RotationY.h>
 
using namespace Belle2;

static double s_InvariantMass;

static double s_InvariantMassError;

static TVector3 s_BoostVector;

static TMatrixDSym s_BoostVectorInverseCovariance(3);

static TVector3 s_DirectionHER;

static TVector3 s_DirectionLER;

static double s_AngleError;

static ROOT::Math::PxPyPzEVector getMomentum(double energy, double thetaX, double thetaY,
                                             bool ler)
{
  const double pz = std::sqrt(energy * energy -
                              Const::electronMass * Const::electronMass);
  const double sx = sin(thetaX);
  const double cx = cos(thetaX);
  const double sy = sin(thetaY);
  const double cy = cos(thetaY);
  const double px = sy * cx * pz;
  const double py = -sx * pz;
  ROOT::Math::PxPyPzEVector result(px, py, cx * cy * pz, energy);
  if (ler) {
    ROOT::Math::RotationY rotationY(M_PI);
    result = rotationY(result);
  }
  return result;
}
 
static void fcn(int& npar, double* grad, double& fval, double* par, int iflag)
{
  (void)npar;
  (void)grad;
  (void)iflag;
  ROOT::Math::PxPyPzEVector pHER, pLER;
  pHER = getMomentum(par[0], par[1], par[2], false);
  pLER = getMomentum(par[3], par[4], par[5], true);
  ROOT::Math::PxPyPzEVector pBeam = pHER + pLER;
  ROOT::Math::XYZVector beamBoost = pBeam.BoostToCM();
  TVectorD boostDifference(3);
  boostDifference[0] = beamBoost.X() - s_BoostVector.X();
  boostDifference[1] = beamBoost.Y() - s_BoostVector.Y();
  boostDifference[2] = beamBoost.Z() - s_BoostVector.Z();
  double boostChi2 = s_BoostVectorInverseCovariance.Similarity(boostDifference);
  double invariantMass = pBeam.M();
  double massChi2 = pow((invariantMass - s_InvariantMass) /
                        s_InvariantMassError, 2);
  double angleHER = ROOT::Math::VectorUtil::Angle(pHER, s_DirectionHER);
  double angleLER = ROOT::Math::VectorUtil::Angle(pLER, s_DirectionLER);
  double angleChi2 = pow(angleHER / s_AngleError, 2) +
                     pow(angleLER / s_AngleError, 2);
  fval = boostChi2 + massChi2 + angleChi2;
}
 
void BeamParametersFitter::setupDatabase()
{
  /* DataStore. */
  DataStore::Instance().setInitializeActive(true);
  StoreObjPtr<EventMetaData> eventMetaData;
  eventMetaData.registerInDataStore();
  DataStore::Instance().setInitializeActive(false);
  /* Database. */
  if (eventMetaData.isValid()) {
    eventMetaData->setExperiment(m_IntervalOfValidity.getExperimentLow());
    eventMetaData->setRun(m_IntervalOfValidity.getRunLow());
  } else {
    eventMetaData.construct(1, m_IntervalOfValidity.getRunLow(),
                            m_IntervalOfValidity.getExperimentLow());
  }
  DBStore& dbStore = DBStore::Instance();
  dbStore.update();
  dbStore.updateEvent();
}
 
/*
 
 In BeamParameters, the momenta are represented as (E, theta_x, theta_y).
The cartesian coordinates of the momenta are given by
 
 |p_x|   |cos(theta_y)  0 sin(theta_y)|   | 1 0            0             |
 |p_y| = |0             1 0           | * | 0 cos(theta_x) -sin(theta_x) |
 |p_x|   |-sin(theta_y) 0 cos(theta_y)|   | 0 sin(theta_x) cos(theta_x)  |
 
           | 0 |
         * | 0 | ,
           | p |
 
or, after, matrix multiplication,
 
 p_x = p * cos(theta_x) * sin(theta_y) ,
 p_y = - p * sin(theta_x) ,
 p_z = p * cos(theta_x) * cos(theta_y) .
 
 The block form of the full covariance matrix is
 
    | V_HER | 0     |
V = |-------|-------| ,
    | 0     | V_LER |
 
where V_HER and V_LER are the covariance matrices of high-energy and
low-energy beam momenta. The directions are assumed to be known exactly,
thus, the covariance matrix has only two non-zero elements:
V_11 = sigma_{E_HER}^2 and V_44 = sigma_{E_LER}^2.
 
 It is necessary to reproduce the measured variance (note that error represents
energy spread rather than the uncertainty of the mean energy) of collision
invariant mass. The corresponding 1x1 error matrix is given by
 
               | \partial \sqrt{s} |       | \partial \sqrt{s} | ^ T
V_{\sqrt{s}} = | ----------------- | * V * | ----------------- |     .
               | \partial p_i      |       | \partial p_i      |
 
Since there are only two non-zero elements, this formula reduces to
 
                      | \partial \sqrt{s} | ^ 2
\sigma^2_{\sqrt{s}} = | ----------------- |     * sigma_{E_HER}^2
                      | \partial E_HER    |
 
                        | \partial \sqrt{s} | ^ 2
                      + | ----------------- |     * sigma_{E_LER}^2 .
                        | \partial E_LER    |
 
 The derivatives are given by
 
\partial \sqrt{s}
----------------- =
 \partial E_HER
 
      1                                                          E_HER
= -------- [ E_beam - (p_beam)_x * cos(theta_x) * sin(theta_y) * -----
  \sqrt{s}                                                       p_HER
 
                                           E_HER
             + (p_beam)_y * sin(theta_x) * -----
                                           p_HER
 
                                                          E_HER
             - (p_beam)_z * cos(theta_x) * cos(theta_y) * ----- ],
                                                          p_HER
 
and by similar formula for E_LER.
 
 Now it is necessary to make some assumption about the relation between
sigma_{E_HER} and sigma_{E_LER}. It is assumed that sigma_{E_HER} = k E_HER
and sigma_{E_LER} = k E_LER.
 
*/
void BeamParametersFitter::fit()
{
  int minuitResult;
  setupDatabase();
  /* Get p_HER and p_LER from a fit. */
  double herMomentum, herThetaX, herThetaY;
  double lerMomentum, lerThetaX, lerThetaY;
  s_BoostVector = m_CollisionBoostVector->getBoost();
  s_BoostVectorInverseCovariance = m_CollisionBoostVector->getBoostCovariance();
  if (s_BoostVectorInverseCovariance.Determinant() == 0) {
    B2WARNING("Determinant of boost covariance matrix is 0, "
              "using generic inverse covariance matrix for fit.");
    s_BoostVectorInverseCovariance[0][0] = 1.0 / (m_BoostError * m_BoostError);
    s_BoostVectorInverseCovariance[0][1] = 0;
    s_BoostVectorInverseCovariance[0][2] = 0;
    s_BoostVectorInverseCovariance[1][0] = 0;
    s_BoostVectorInverseCovariance[1][1] = 1.0 / (m_BoostError * m_BoostError);
    s_BoostVectorInverseCovariance[1][2] = 0;
    s_BoostVectorInverseCovariance[2][0] = 0;
    s_BoostVectorInverseCovariance[2][1] = 0;
    s_BoostVectorInverseCovariance[2][2] = 1.0 / (m_BoostError * m_BoostError);
  } else {
    s_BoostVectorInverseCovariance.Invert();
  }
  s_InvariantMass = m_CollisionInvariantMass->getMass();
  s_InvariantMassError = m_CollisionInvariantMass->getMassError();
  if (s_InvariantMassError == 0) {
    B2WARNING("Invariant-mass errror is 0, using generic error for fit.");
    s_InvariantMassError = m_InvariantMassError;
  }
  s_DirectionHER.SetX(0);
  s_DirectionHER.SetY(0);
  s_DirectionHER.SetZ(1);
  s_DirectionHER.RotateY(m_AngleHER);
  s_DirectionLER.SetX(0);
  s_DirectionLER.SetY(0);
  s_DirectionLER.SetZ(1);
  s_DirectionLER.RotateY(m_AngleLER + M_PI);
  s_AngleError = m_AngleError;
  TMinuit minuit(6);
  if (!m_Verbose)
    minuit.SetPrintLevel(-1);
  minuit.SetFCN(fcn);
  minuit.mnparm(0, "PHER_E", 7, 0.01, 0, 0, minuitResult);
  minuit.mnparm(1, "PHER_TX", 0, 0.01, 0, 0, minuitResult);
  minuit.mnparm(2, "PHER_TY", 0, 0.01, 0, 0, minuitResult);
  minuit.mnparm(3, "PLER_E", 4, 0.01, 0, 0, minuitResult);
  minuit.mnparm(4, "PLER_TX", 0, 0.01, 0, 0, minuitResult);
  minuit.mnparm(5, "PLER_TY", 0, 0.01, 0, 0, minuitResult);
  minuit.mncomd("FIX 2 3 5 6", minuitResult);
  minuit.mncomd("MIGRAD 10000", minuitResult);
  minuit.mncomd("RELEASE 2 3 5 6", minuitResult);
  minuit.mncomd("MIGRAD 10000", minuitResult);
  double error;
  minuit.GetParameter(0, herMomentum, error);
  minuit.GetParameter(1, herThetaX, error);
  minuit.GetParameter(2, herThetaY, error);
  minuit.GetParameter(3, lerMomentum, error);
  minuit.GetParameter(4, lerThetaX, error);
  minuit.GetParameter(5, lerThetaY, error);
  /* Calculate error. */
  ROOT::Math::PxPyPzEVector pHER = getMomentum(herMomentum, herThetaX, herThetaY, false);
  ROOT::Math::PxPyPzEVector pLER = getMomentum(lerMomentum, lerThetaX, lerThetaY, true);
  ROOT::Math::PxPyPzEVector pBeam = pHER + pLER;
  double fittedInvariantMass = pBeam.M();
  B2RESULT("Initial invariant mass: " << s_InvariantMass <<
           "; fitted invariant mass: " << fittedInvariantMass);
  double cosThetaX = cos(herThetaX);
  double sinThetaX = sin(herThetaX);
  double cosThetaY = cos(herThetaY);
  double sinThetaY = sin(herThetaY);
  double herPartial =
    (pBeam.E() - pHER.E() / pHER.P() *
     (pBeam.Px() * cosThetaX * sinThetaY - pBeam.Py() * sinThetaX +
      pBeam.Pz() * cosThetaX * cosThetaY)) / fittedInvariantMass;
  cosThetaX = cos(lerThetaX);
  sinThetaX = sin(lerThetaX);
  cosThetaY = cos(lerThetaY + M_PI);
  sinThetaY = sin(lerThetaY + M_PI);
  double lerPartial =
    (pBeam.E() - pLER.E() / pLER.P() *
     (pBeam.Px() * cosThetaX * sinThetaY - pBeam.Py() * sinThetaX +
      pBeam.Pz() * cosThetaX * cosThetaY)) / fittedInvariantMass;
  double sigmaInvariantMass = m_CollisionInvariantMass->getMassSpread();
  double k = sqrt(sigmaInvariantMass * sigmaInvariantMass /
                  (pow(herPartial * pHER.E(), 2) +
                   pow(lerPartial * pLER.E(), 2)));
  double herSpread = k * pHER.E();
  double lerSpread = k * pLER.E();
  B2INFO("Invariant mass spread: " << sigmaInvariantMass);
  B2RESULT("HER energy spread: " << herSpread <<
           "; LER energy spread: " << lerSpread);
  /* Fill beam parameters. */
  m_BeamParameters.setHER(pHER);
  m_BeamParameters.setLER(pLER);
  TMatrixDSym covariance(3);
  for (int i = 0; i < 3; ++i) {
    for (int j = 0; j < 3; ++j)
      covariance[i][j] = 0;
  }
  covariance[0][0] = herSpread * herSpread;
  m_BeamParameters.setCovHER(covariance);
  covariance[0][0] = lerSpread * lerSpread;
  m_BeamParameters.setCovLER(covariance);
}
 
void BeamParametersFitter::fillVertexData(
  double covarianceXX, double covarianceYY)
{
  setupDatabase();
  m_BeamParameters.setVertex(ROOT::Math::XYZVector(m_BeamSpot->getIPPosition()));
  TMatrixDSym beamSize = m_BeamSpot->getSizeCovMatrix();
  double xScale, yScale;
  if (covarianceXX < 0)
    xScale = 1;
  else
    xScale = sqrt(covarianceXX / beamSize[0][0]);
  if (covarianceYY < 0)
    yScale = 1;
  else
    yScale = sqrt(covarianceYY / beamSize[1][1]);
  for (int i = 0; i < 3; ++i) {
    beamSize[0][i] *= xScale;
    beamSize[i][0] *= xScale;
    beamSize[1][i] *= yScale;
    beamSize[i][1] *= yScale;
  }
  m_BeamParameters.setCovVertex(beamSize);
}
 
void BeamParametersFitter::importBeamParameters()
{
  DBImportObjPtr<BeamParameters> beamParametersImport;
  beamParametersImport.construct(m_BeamParameters);
  beamParametersImport.import(m_IntervalOfValidity);
}