TRTProcessingOfStraw Class Reference

TRT Digitization: Processing of a TRT Straws. More...

#include <TRTProcessingOfStraw.h>

Inheritance diagram for TRTProcessingOfStraw:

Collaboration diagram for TRTProcessingOfStraw:

Classes
class	cluster
	Primary ionisation cluster. More...

Public Types
typedef TimedHitCollection< TRTUncompressedHit >::const_iterator	hitCollConstIter

Public Member Functions
	TRTProcessingOfStraw (const TRTDigSettings *, const InDetDD::TRT_DetectorManager *, ITRT_PAITool *, ITRT_SimDriftTimeTool *, TRTElectronicsProcessing *ep, TRTNoise *noise, TRTDigCondBase *digcond, const HepPDT::ParticleDataTable *, const TRT_ID *, ITRT_PAITool *=nullptr, ITRT_PAITool *=nullptr, const ITRT_CalDbTool *=nullptr)
	Constructor: Calls Initialize method. More...
	~TRTProcessingOfStraw ()
	Destructor. More...
void	ProcessStraw (MagField::AtlasFieldCache &fieldCache, hitCollConstIter i, hitCollConstIter e, TRTDigit &outdigit, bool &m_alreadyPrintedPDGcodeWarning, double m_cosmicEventPhase, int strawGasType, bool emulationArflag, bool emulationKrflag, CLHEP::HepRandomEngine *rndmEngine, CLHEP::HepRandomEngine *elecProcRndmEngine, CLHEP::HepRandomEngine *elecNoiseRndmEngine, CLHEP::HepRandomEngine *paiRndmEngine)
	Process this straw all the way from Geant4 hit to output digit. More...
bool	msgLvl (const MSG::Level lvl) const
	Test the output level. More...
MsgStream &	msg () const
	The standard message stream. More...
MsgStream &	msg (const MSG::Level lvl) const
	The standard message stream. More...
void	setLevel (MSG::Level lvl)
	Change the current logging level. More...

Protected Attributes
const TRT_ID *	m_id_helper

Private Member Functions
	TRTProcessingOfStraw (const TRTProcessingOfStraw &)
TRTProcessingOfStraw &	operator= (const TRTProcessingOfStraw &)
void	Initialize (const ITRT_CalDbTool *)
	Initialize. More...
void	addClustersFromStep (const double &scaledKineticEnergy, const double &particleCharge, const double &timeOfHit, const double &prex, const double &prey, const double &prez, const double &postx, const double &posty, const double &postz, std::vector< cluster > &clusterlist, int strawGasType, CLHEP::HepRandomEngine *rndmEngine, CLHEP::HepRandomEngine *paiRndmEngine)
	This is the main function for re-simulation of the ionisation in the active gas via the PAI model. More...
void	ClustersToDeposits (MagField::AtlasFieldCache &fieldCache, const int &hitID, const std::vector< cluster > &clusters, std::vector< TRTElectronicsProcessing::Deposit > &deposits, Amg::Vector3D TRThitGlobalPos, double m_cosmicEventPhase, int strawGasType, CLHEP::HepRandomEngine *rndmEngine)
	Transform the ioniation clusters along the particle trajectory inside a straw to energy deposits (i.e. More...
double	setClusterZ (double cluster_z_in, bool isLong, bool isShort, bool isEC) const
Amg::Vector3D	getGlobalPosition (int hitID, const TimedHitPtr< TRTUncompressedHit > *theHit)
void	initMessaging () const
	Initialize our message level and MessageSvc. More...

Private Attributes
const TRTDigSettings *	m_settings
const InDetDD::TRT_DetectorManager *	m_detmgr
ITRT_PAITool *	m_pPAItoolXe
ITRT_PAITool *	m_pPAItoolAr
ITRT_PAITool *	m_pPAItoolKr
ITRT_SimDriftTimeTool *	m_pSimDriftTimeTool
bool	m_timeCorrection = false
	Time to be corrected for flight and wire propagation delays false when beamType='cosmics'. More...
double	m_signalPropagationSpeed = 0.0
double	m_attenuationLength = 0.0
bool	m_useAttenuation = false
bool	m_useMagneticFieldMap = false
double	m_maxCrossingTime = 0.0
double	m_minCrossingTime = 0.0
double	m_shiftOfZeroPoint = 0.0
double	m_innerRadiusOfStraw = 0.0
double	m_outerRadiusOfWire = 0.0
double	m_solenoidFieldStrength = 0.0
TRTTimeCorrection *	m_pTimeCorrection
TRTElectronicsProcessing *	m_pElectronicsProcessing
TRTNoise *	m_pNoise
TRTDigCondBase *	m_pDigConditions
const HepPDT::ParticleDataTable *	m_pParticleTable
std::vector< cluster >	m_clusterlist
std::vector< TRTElectronicsProcessing::Deposit >	m_depositList
std::vector< double >	m_drifttimes
std::vector< double >	m_expattenuation
unsigned int	m_maxelectrons = 0U
bool	m_alreadywarnedagainstpdg0
std::unique_ptr< CLHEP::RandBinomialFixedP >	m_randBinomialXe {}
std::unique_ptr< CLHEP::RandBinomialFixedP >	m_randBinomialKr {}
std::unique_ptr< CLHEP::RandBinomialFixedP >	m_randBinomialAr {}
std::string	m_nm
	Message source name. More...
boost::thread_specific_ptr< MsgStream >	m_msg_tls
	MsgStream instance (a std::cout like with print-out levels) More...
std::atomic< IMessageSvc * >	m_imsg { nullptr }
	MessageSvc pointer. More...
std::atomic< MSG::Level >	m_lvl { MSG::NIL }
	Current logging level. More...
std::atomic_flag m_initialized	ATLAS_THREAD_SAFE = ATOMIC_FLAG_INIT
	Messaging initialized (initMessaging) More...

Detailed Description

TRT Digitization: Processing of a TRT Straws.

The main controlling function in ProcessStraw(). See detailed description of this.

Definition at line 54 of file TRTProcessingOfStraw.h.

Member Typedef Documentation

hitCollConstIter

typedef TimedHitCollection<TRTUncompressedHit>::const_iterator TRTProcessingOfStraw::hitCollConstIter

Definition at line 73 of file TRTProcessingOfStraw.h.

Constructor & Destructor Documentation

TRTProcessingOfStraw() [1/2]

TRTProcessingOfStraw::TRTProcessingOfStraw	(	const TRTDigSettings *	digset,
		const InDetDD::TRT_DetectorManager *	detmgr,
		ITRT_PAITool *	paitoolXe,
		ITRT_SimDriftTimeTool *	simdrifttool,
		TRTElectronicsProcessing *	ep,
		TRTNoise *	noise,
		TRTDigCondBase *	digcond,
		const HepPDT::ParticleDataTable *	pdt,
		const TRT_ID *	trt_id,
		ITRT_PAITool *	paitoolAr = nullptr,
		ITRT_PAITool *	paitoolKr = nullptr,
		const ITRT_CalDbTool *	calDbTool = nullptr
	)

Constructor: Calls Initialize method.

Definition at line 48 of file TRTProcessingOfStraw.cxx.

: AthMessaging("TRTProcessingOfStraw"),
  m_settings(digset),
  m_detmgr(detmgr),
  m_pPAItoolXe(paitoolXe),
  m_pPAItoolAr(paitoolAr),
  m_pPAItoolKr(paitoolKr),
  m_pSimDriftTimeTool(simdrifttool),
// m_time_y_eq_zero(0.0),
// m_ComTime(NULL),
  m_pTimeCorrection(nullptr),
  m_pElectronicsProcessing(ep),
  m_pNoise(noise),
  m_pDigConditions(digcond),
  m_pParticleTable(pdt),
  m_alreadywarnedagainstpdg0(false),
  m_id_helper(trt_id)
 
{
  Initialize(calDbTool);
}

~TRTProcessingOfStraw()

TRTProcessingOfStraw::~TRTProcessingOfStraw

(

)

Destructor.

Definition at line 83 of file TRTProcessingOfStraw.cxx.

{
  delete m_pTimeCorrection;
}

TRTProcessingOfStraw() [2/2]

TRTProcessingOfStraw::TRTProcessingOfStraw ( const TRTProcessingOfStraw &  )

private

Member Function Documentation

addClustersFromStep()

void TRTProcessingOfStraw::addClustersFromStep ( const double &  scaledKineticEnergy, const double &  particleCharge, const double &  timeOfHit, const double &  prex, const double &  prey, const double &  prez, const double &  postx, const double &  posty, const double &  postz, std::vector< cluster > &  clusterlist, int  strawGasType, CLHEP::HepRandomEngine *  rndmEngine, CLHEP::HepRandomEngine *  paiRndmEngine  )

private

This is the main function for re-simulation of the ionisation in the active gas via the PAI model.

From the given G4 step, ionisation clusters are distributed randomly (mean free path given by TRT_PAI_Process::GetMeanFreePath()) along path. Cluster energies are given by TRT_PAI_Process::GetEnergyTransfer().

Parameters

scaledKineticEnergy	The kinetic energy a proton would have had if it had the same Lorentz gamma factor as the particle in question.
particleCharge	Particle charge
timeOfHit	Time of hit
prex	PreStepPoint x coordinate
prey	PreStepPoint y coordinate
prez	PreStepPoint z coordinate
postx	PostStepPoint x coordinate
posty	PostStepPoint y coordinate
postz	PostStepPoint z coordinate
clusterlist	List of ionisation clusters along step

Definition at line 204 of file TRTProcessingOfStraw.cxx.

{
 
  // Choose the appropriate ITRT_PAITool for this straw
  ITRT_PAITool* activePAITool;
  if      (strawGasType==0) { activePAITool = m_pPAItoolXe; }
  else if (strawGasType==1) { activePAITool = m_pPAItoolKr; }
  else if (strawGasType==2) { activePAITool = m_pPAItoolAr; }
  else { activePAITool = m_pPAItoolXe; } // should never happen
 
  //Differences and steplength:
  const double deltaX(postx - prex);
  const double deltaY(posty - prey);
  const double deltaZ(postz - prez);
  const double stepLength(sqrt(deltaX * deltaX + deltaY * deltaY + deltaZ * deltaZ));
 
  const double meanFreePath(activePAITool->GetMeanFreePath( scaledKineticEnergy, particleCharge*particleCharge ));
 
  //How many clusters did we actually create:
  const unsigned int numberOfClusters(CLHEP::RandPoisson::shoot(rndmEngine,stepLength / meanFreePath));
  //fixme: use RandPoissionQ?
 
  //Position each of those randomly along the step, and use PAI to get their energies:
  for (unsigned int iclus(0); iclus<numberOfClusters; ++iclus)
    {
      //How far along the step did the cluster get produced:
      const double lambda(CLHEP::RandFlat::shoot(rndmEngine));
 
      //Append cluster (the energy is given by the PAI model):
      double clusE(activePAITool->GetEnergyTransfer(scaledKineticEnergy, paiRndmEngine));
      clusterlist.emplace_back(clusE, timeOfHit,
                                    prex + lambda * deltaX,
                                    prey + lambda * deltaY,
                                    prez + lambda * deltaZ);
    }
 
  
}

ClustersToDeposits()

void TRTProcessingOfStraw::ClustersToDeposits ( MagField::AtlasFieldCache &  fieldCache, const int &  hitID, const std::vector< cluster > &  clusters, std::vector< TRTElectronicsProcessing::Deposit > &  deposits, Amg::Vector3D  TRThitGlobalPos, double  m_cosmicEventPhase, int  strawGasType, CLHEP::HepRandomEngine *  rndmEngine  )

private

Transform the ioniation clusters along the particle trajectory inside a straw to energy deposits (i.e.

potential fluctuations) reaching the front-end electronics. Effects taken into effect are:

• number of primary electrons from deposited energy
• stocastic recapture of drift electrons
• electron drift in the magnetic field (different direction end-cap/barrel). Optionally the drift time includes spread.
• Optionally signal wire propagation dealys are included. Each drift electron then gives rise to two signal: direct and reflected.

Parameters

hitID	Id of straw
clusters	ionisation clusters along particle trajectory
deposits	energy deposits on wire

Definition at line 521 of file TRTProcessingOfStraw.cxx.

{
 
  //
  // Some initial work before looping over the cluster
  //
 
  deposits.clear();
 
  unsigned int region(TRTDigiHelper::getRegion(hitID));
  const bool isBarrel(region<3 );
  const bool isEC    (!isBarrel);
  const bool isShort (region==1);
  const bool isLong  (region==2);
  //const bool isECA   (region==3);
  //const bool isECB   (region==4);
 
  CLHEP::RandBinomialFixedP *randBinomial{};
  if      (strawGasType == 0) { randBinomial = m_randBinomialXe.get(); }
  else if (strawGasType == 1) { randBinomial = m_randBinomialKr.get(); }
  else if (strawGasType == 2) { randBinomial = m_randBinomialAr.get(); }
  else { randBinomial = m_randBinomialXe.get(); } // should never happen
 
  double ionisationPotential = m_settings->ionisationPotential(strawGasType);
  double smearingFactor      = m_settings->smearingFactor(strawGasType);
 
  std::vector<cluster>::const_iterator currentClusterIter(clusters.begin());
  const std::vector<cluster>::const_iterator endOfClusterList(clusters.end());
 
  // if (m_settings->doCosmicTimingPit()) {
  //     if (m_ComTime) { m_time_y_eq_zero = m_ComTime->getTime(); }
  //     else           { ATH_MSG_WARNING("Configured to use ComTime tool, but did not find tool. All hits will get the same t0"); }
  // }
 
  // The average drift time is affected by the magnetic field which is not uniform so we need to use the
  // detailed magnetic field map to obtain an effective field for this straw (used in SimDriftTimeTool).
  // This systematically affects O(ns) drift times in the end cap, but has a very small effect in the barrel.
  Amg::Vector3D globalPosition;
  Amg::Vector3D mField;
  double map_x2(0.),map_y2(0.),map_z2(0.);
  double effectiveField2(0.); // effective field squared.
 
  // Magnetic field is the same for all clusters in the straw so this can be called before the cluster loop.
  if (m_useMagneticFieldMap)
    {
      globalPosition[0]=TRThitGlobalPos[0]*CLHEP::mm;
      globalPosition[1]=TRThitGlobalPos[1]*CLHEP::mm;
      globalPosition[2]=TRThitGlobalPos[2]*CLHEP::mm;
 
      // MT Field cache is stored in cache
      fieldCache.getField         (globalPosition.data(), mField.data());
 
      map_x2 = mField.x()*mField.x(); // would be zero for a uniform field
      map_y2 = mField.y()*mField.y(); // would be zero for a uniform field
      map_z2 = mField.z()*mField.z(); // would be m_solenoidfieldstrength^2 for uniform field
    }
 
  // Now we are ready to loop over clusters and form timed energy deposits at the wire:
  //
  //  1. First determine the number of surviving drift electrons and the energy of their deposits.
  //  2. Then determine the timing of these deposits.
 
  // Notes
  //
  // 1) It turns out that the total energy deposited (Ed) is, on average, equal to the cluster energy (Ec):
  // <Ed> = m_ionisationPotential/m_smearingFactor * Ec/m_ionisationPotential * m_smearingFactor = Ec.
  // Actually it exceeds this *slightly* due to the +1 electron in the calculation of nprimaryelectrons below.
  // The energy processing below therefore exists only to model the energy *fluctuations*.
  //
  // 2) Gaussian approximation (for photons, HIPs etc):
  // For large Ec (actually nprimaryelectrons > 99) a much faster Gaussian shoot replaces
  // the Binomial and many exponential shoots. The Gaussian pdf has a mean of Ec and variance
  // given by sigma^2 = Ec*ionisationPotential*(2-smearingFactor)/smearingFactor. That expression
  // comes from the sum of the variances from the Binomial and Exponential. In this scheme it is
  // sufficient (for diffusion) to divided the energy equally amongst 100 (maxelectrons) electrons.
 
  // straw radius
  const double  wire_r2 = m_outerRadiusOfWire*m_outerRadiusOfWire;
  const double straw_r2 = m_innerRadiusOfStraw*m_innerRadiusOfStraw;
 
  // Cluster loop
  for (;currentClusterIter!=endOfClusterList;++currentClusterIter)
    {
      // Get the cluster radius and energy.
      const double cluster_x(currentClusterIter->xpos);
      const double cluster_y(currentClusterIter->ypos);
      const double cluster_z(this->setClusterZ(currentClusterIter->zpos, isLong, isShort, isEC));
      const double cluster_x2(cluster_x*cluster_x);
      const double cluster_y2(cluster_y*cluster_y);
      double cluster_r2(cluster_x2+cluster_y2);
 
      // These may never occur, but could be very problematic for getAverageDriftTime(), so check and correct this now.
      if (cluster_r2<wire_r2)  cluster_r2=wire_r2;  // Compression may (v. rarely) cause r to be smaller than the wire radius. If r=0 then NaN's later!
      if (cluster_r2>straw_r2) cluster_r2=straw_r2; // Should never occur
 
      const double cluster_r(std::sqrt(cluster_r2));      // cluster radius
      const double cluster_E(currentClusterIter->energy); // cluster energy
      const unsigned int nprimaryelectrons( static_cast<unsigned int>( cluster_E / ionisationPotential + 1.0 ) );
 
      // Determine the number of surviving electrons and their energy sum.
      // If nprimaryelectrons > 100 then a Gaussian approximation is good (and much quicker)
 
      double depositEnergy(0.); // This will be the energy deposited at the wire.
 
      if (nprimaryelectrons<m_maxelectrons) // Use the detailed Binomial and Exponential treatment at this low energy.
        {
          unsigned int nsurvivingprimaryelectrons = static_cast<unsigned int>(randBinomial->fire(rndmEngine,nprimaryelectrons) + 0.5);
          if (nsurvivingprimaryelectrons==0) continue; // no electrons survived; move on to the next cluster.
          const double meanElectronEnergy(ionisationPotential / smearingFactor);
          for (unsigned int ielec(0); ielec<nsurvivingprimaryelectrons; ++ielec) {
            depositEnergy += CLHEP::RandExpZiggurat::shoot(rndmEngine, meanElectronEnergy);
          }
        }
      else // Use a Gaussian approximation
        {
          const double fluctSigma(sqrt(cluster_E * ionisationPotential * (2 - smearingFactor) / smearingFactor));
          do {
            depositEnergy = CLHEP::RandGaussZiggurat::shoot(rndmEngine, cluster_E, fluctSigma);
          } while(depositEnergy<0.0); // very rare.
        }
 
      // Now we have the depositEnergy, we need to work out the timing and attenuation
 
      // First calculate the "effective field" (it's never negative):
      // Electron drift time is prolonged by the magnetic field according to an "effective field".
      // For the endcap, the effective field is dependent on the relative (x,y) position of the cluster.
      // It is assumed here (checked in initialize) that the local straw x-direction is parallel with
      // the solenoid z-direction. After Garfield simulations and long thought it was found that only
      // field perpendicular to the electron drift is of importance.
 
      if (!isBarrel) // Endcap
        {
          if (m_useMagneticFieldMap) { // Using magnetic field map
            effectiveField2 = map_z2*cluster_y2/cluster_r2 + map_x2 + map_y2;
          }
          else { // Not using magnetic field map (you really should not do this!):
            effectiveField2 = m_solenoidFieldStrength*m_solenoidFieldStrength * cluster_y2 / cluster_r2;
          }
        }
      else // Barrel
        {
          if (m_useMagneticFieldMap) { // Using magnetic field map (here bug #91830 is corrected)
            effectiveField2 = map_z2 + (map_x2+map_y2)*cluster_y2/cluster_r2;
          }
          else { // Without the mag field map (very small change in digi output)
            effectiveField2 = m_solenoidFieldStrength*m_solenoidFieldStrength;
          }
        }
 
      // If there is no field we might need to reset effectiveField2 to zero.
      if (m_solenoidFieldStrength == 0. ) effectiveField2=0.;
 
      // Now we need the deposit time which is the sum of three components:
      // 1. Time of the hit(cluster): clusterTime.
      // 2. Drift times: either commondrifttime, or diffused m_drifttimes
      // 3. Wire propagation times: timedirect and timereflect.
 
      // get the time of the hit(cluster)
      double clusterTime(currentClusterIter->time);
 
      if ( m_settings->doCosmicTimingPit() )
        { // make (x,y) dependent? i.e: + f(x,y).
          // clusterTime = clusterTime - m_time_y_eq_zero + m_settings->jitterTimeOffset()*( CLHEP::RandFlat::shoot(rndmEngine) );
          clusterTime = clusterTime + cosmicEventPhase + m_settings->jitterTimeOffset()*( CLHEP::RandFlat::shoot(rndmEngine) );
          // yes it is a '+' now. Ask Alex Alonso.
        }
 
      // get the wire propagation times (for direct and reflected signals)
      double timedirect(0.), timereflect(0.);
      m_pTimeCorrection->PropagationTime( hitID, cluster_z, timedirect, timereflect );
 
      // While we have the propagation times, we can calculate the exponential attenuation factor
      double expdirect(1.0), expreflect(1.0); // Initially set to "no attenuation".
      if (m_useAttenuation)
        {
          //expdirect  = exp( -timedirect *m_signalPropagationSpeed / m_attenuationLength);
          //expreflect = exp( -timereflect*m_signalPropagationSpeed / m_attenuationLength);
          // Tabulating exp(-dist/m_attenuationLength) with only 150 elements: index [0,149].
          //   > 99.9% of output digits are the same, saves 13% CPU time.
          // Distances the signal propagate along the wire:
          // * distdirect is rarely negative (<0.2%) by ~ mm. In such cases there is
          //   no attenuation, which is equivalent to distdirect=0 and so is good.
          // * distreflect is always +ve and less than 1500, and so is good.
          // The code is protected against out of bounds in anycase.
          const double distdirect  = timedirect *m_signalPropagationSpeed;
          const double distreflect = timereflect*m_signalPropagationSpeed;
          const unsigned int kdirect  = static_cast<unsigned int>(distdirect/10);
          const unsigned int kreflect = static_cast<unsigned int>(distreflect/10);
          if (kdirect<150) expdirect  = m_expattenuation[kdirect];    // otherwise there
          if (kreflect<150) expreflect = m_expattenuation[kreflect];  // is no attenuation.
        }
 
      // Finally, deposit the energy on the wire using the drift-time tool (diffusion is no longer available).
      double commondrifttime = m_pSimDriftTimeTool->getAverageDriftTime(cluster_r,effectiveField2,strawGasType);
      double dt = clusterTime + commondrifttime;
      deposits.emplace_back(0.5*depositEnergy*expdirect,  timedirect+dt);
      deposits.emplace_back(0.5*depositEnergy*expreflect, timereflect+dt);
 
    } // end of cluster loop
 
  }

getGlobalPosition()

Amg::Vector3D TRTProcessingOfStraw::getGlobalPosition ( int  hitID, const TimedHitPtr< TRTUncompressedHit > *  theHit  )

private

Definition at line 730 of file TRTProcessingOfStraw.cxx.

                                                                                                                {
 
  const int mask(0x0000001F);
  int word_shift(5);
  int trtID, ringID, moduleID, layerID, strawID;
  int wheelID, planeID, sectorID;
 
  const InDetDD::TRT_BarrelElement *barrelElement;
  const InDetDD::TRT_EndcapElement *endcapElement;
 
  if ( !(hitID & 0x00200000) ) {      // barrel
 
    strawID   = hitID & mask;
    hitID   >>= word_shift;
    layerID   = hitID & mask;
    hitID   >>= word_shift;
    moduleID  = hitID & mask;
    hitID   >>= word_shift;
    ringID    = hitID & mask;
    trtID     = hitID >> word_shift;
 
    barrelElement = m_detmgr->getBarrelElement(trtID, ringID, moduleID, layerID);
 
    if (barrelElement) {
      const Amg::Vector3D v( (*theHit)->GetPreStepX(),(*theHit)->GetPreStepY(),(*theHit)->GetPreStepZ());
      return barrelElement->strawTransform(strawID)*v;
    }
 
  } else {                           // endcap
 
    strawID   = hitID & mask;
    hitID   >>= word_shift;
    planeID   = hitID & mask;
    hitID   >>= word_shift;
    sectorID  = hitID & mask;
    hitID   >>= word_shift;
    wheelID   = hitID & mask;
    trtID     = hitID >> word_shift;
 
    // change trtID (which is 2/3 for endcaps) to use 0/1 in getEndcapElement
    if (trtID == 3) trtID = 0;
    else            trtID = 1;
 
    endcapElement = m_detmgr->getEndcapElement(trtID, wheelID, planeID, sectorID);
 
    if ( endcapElement ) {
      const Amg::Vector3D v( (*theHit)->GetPreStepX(),(*theHit)->GetPreStepY(),(*theHit)->GetPreStepZ());
      return endcapElement->strawTransform(strawID)*v;
    }
 
  }
 
  ATH_MSG_WARNING ( "Could not find global coordinate of a straw - drifttime calculation will be inaccurate" );
  return {0.0,0.0,0.0};
 
}

Initialize()

void TRTProcessingOfStraw::Initialize ( const ITRT_CalDbTool *  calDbTool )

private

Initialize.

Definition at line 89 of file TRTProcessingOfStraw.cxx.

{
 
  m_useMagneticFieldMap    = m_settings->useMagneticFieldMap();
  m_signalPropagationSpeed = m_settings->signalPropagationSpeed() ;
  m_attenuationLength      = m_settings->attenuationLength();
  m_useAttenuation         = m_settings->useAttenuation();
  m_innerRadiusOfStraw     = m_settings->innerRadiusOfStraw();
  m_outerRadiusOfWire      = m_settings->outerRadiusOfWire();
  m_timeCorrection         = m_settings->timeCorrection();        // false for beamType='cosmics'
  m_solenoidFieldStrength  = m_settings->solenoidFieldStrength();
 
  m_maxelectrons = 100; // 100 gives good Gaussian approximation
 
  if (m_pPAItoolXe==nullptr) {
    ATH_MSG_FATAL ( "TRT_PAITool for Xenon not defined! no point in continuing!" );
  }
  if (m_pPAItoolKr==nullptr) {
    ATH_MSG_ERROR ( "TRT_PAITool for Krypton is not defined!!! Xenon TRT_PAITool will be used for Krypton straws!" );
    m_pPAItoolKr = m_pPAItoolXe;
  }
  if (m_pPAItoolAr==nullptr) {
    ATH_MSG_ERROR ( "TRT_PAITool for Argon is not defined!!! Xenon TRT_PAITool will be used for Argon straws!" );
    m_pPAItoolAr = m_pPAItoolXe;
  }
 
  ATH_MSG_INFO ( "Xe barrel drift-time at r = 2 mm is " << m_pSimDriftTimeTool->getAverageDriftTime(2.0, 0.002*0.002, 0) << " ns." );
  ATH_MSG_INFO ( "Kr barrel drift-time at r = 2 mm is " << m_pSimDriftTimeTool->getAverageDriftTime(2.0, 0.002*0.002, 1) << " ns." );
  ATH_MSG_INFO ( "Ar barrel drift-time at r = 2 mm is " << m_pSimDriftTimeTool->getAverageDriftTime(2.0, 0.002*0.002, 2) << " ns." );
 
  m_pTimeCorrection = new TRTTimeCorrection(m_settings, m_detmgr, m_id_helper, calDbTool);
 
  const double intervalBetweenCrossings(m_settings->timeInterval() / 3.);
  m_minCrossingTime = - (intervalBetweenCrossings * 2. + 1.*CLHEP::ns);
  m_maxCrossingTime =    intervalBetweenCrossings * 3. + 1.*CLHEP::ns;
  m_shiftOfZeroPoint = static_cast<double>( m_settings->numberOfCrossingsBeforeMain() ) * intervalBetweenCrossings;
 
  // Tabulate exp(-dist/m_attenuationLength) as a function of dist = time*m_signalPropagationSpeed [0.0 mm, 1500 mm)
  // otherwise we are doing an exp() for every cluster! > 99.9% of output digits are the same, saves 13% CPU time.
  m_expattenuation.reserve(150);
  for (unsigned int k=0; k<150; k++) {
    double dist = 10.0*(k+0.5); // [5mm, 1415mm] max 5 mm error (sigma = 3 mm)
    m_expattenuation.push_back(exp(-dist/m_attenuationLength));
  }
 
  //For the field effect on drifttimes in this class we will assume that the local x,y coordinates of endcap straws are such that the
  //local y-direction is parallel to the global z-direction. As a sanity check against future code developments we will test this
  //assumption on one straw from each endcap layer.
 
  if (m_solenoidFieldStrength!=0.0)
    {
      const InDetDD::TRT_Numerology * num = m_detmgr->getNumerology();
      for (unsigned int iwheel = 0; iwheel < num->getNEndcapWheels(); ++iwheel)
        {
          for (unsigned int iside = 0; iside < 2; ++iside)
            { //positive and negative endcap
              for (unsigned int ilayer = 0; ilayer < num->getNEndcapLayers(iwheel); ++ilayer)
                {
                  const InDetDD::TRT_EndcapElement * ec_element
                    = m_detmgr->getEndcapElement(iside,//positive or negative endcap
                                                 iwheel,//wheelIndex,
                                                 ilayer,//strawLayerIndex,
                                                 0);//phiIndex
                  //Local straw center and local straw point one unit along x:
                  if (!ec_element)
                    {
                      ATH_MSG_VERBOSE ( "Failed to retrieve endcap element for (iside,iwheel,ilayer)=("
                                        << iside<<", "<<iwheel<<", "<<ilayer<<")." );
                      continue;
                    }
                  Amg::Vector3D strawcenter(0.0,0.0,0.0);
                  Amg::Vector3D strawx(1.0,0.0,0.0);
                  //Transform to global coordinate (use first straw in element):
                  strawcenter = ec_element->strawTransform(0) * strawcenter;
                  strawx = ec_element->strawTransform(0) * strawx;
                  const Amg::Vector3D v(strawx-strawcenter);
                  const double zcoordfrac((v.z()>0?v.z():-v.z())/v.mag());
                  if (zcoordfrac<0.98 || zcoordfrac > 1.02)
                    {
                      ATH_MSG_WARNING ( "Found endcap straw where the assumption that local x-direction"
                                        <<" is parallel to global z-direction is NOT valid."
                                        <<" Drift times will be somewhat off." );
                    }
                }
            }
        }
 
      //check local barrel coordinates at four positions.
      for (unsigned int phi_it = 0; phi_it < 32; phi_it++)
        {
          const InDetDD::TRT_BarrelElement * bar_element = m_detmgr->getBarrelElement(1,1,phi_it,1);
 
          Amg::Vector3D strawcenter(0.0,0.0,0.0);
          Amg::Vector3D straw(cos((double)phi_it*2*M_PI/32.),sin((double)phi_it*2*M_PI/32.),0.0);
          strawcenter = bar_element->strawTransform(0) * strawcenter;
          straw = bar_element->strawTransform(0) * straw;
          const Amg::Vector3D v(straw-strawcenter);
          const double coordfrac(atan2(v.x(),v.y()));
          if (coordfrac>0.2 || coordfrac < -0.2)
            {
              ATH_MSG_WARNING ( "Found barrel straw where the assumption that local y-direction"
                                <<" is along the straw is NOT valid."
                                <<" Drift times will be somewhat off." );
            }
        }
    }
 
  m_randBinomialXe = std::make_unique<CLHEP::RandBinomialFixedP>(nullptr, 1, m_settings->smearingFactor(0), m_maxelectrons);
  m_randBinomialKr = std::make_unique<CLHEP::RandBinomialFixedP>(nullptr, 1, m_settings->smearingFactor(1), m_maxelectrons);
  m_randBinomialAr = std::make_unique<CLHEP::RandBinomialFixedP>(nullptr, 1, m_settings->smearingFactor(2), m_maxelectrons);
 
  ATH_MSG_VERBOSE ( "Initialization done" );
}

initMessaging()

void AthMessaging::initMessaging ( ) const

privateinherited

Initialize our message level and MessageSvc.

This method should only be called once.

Definition at line 39 of file AthMessaging.cxx.

{
  m_imsg = Athena::getMessageSvc();
  m_lvl = m_imsg ?
    static_cast<MSG::Level>( m_imsg.load()->outputLevel(m_nm) ) :
    MSG::INFO;
}

msg() [1/2]

MsgStream & AthMessaging::msg ( ) const

inlineinherited

The standard message stream.

Returns a reference to the default message stream May not be invoked before sysInitialize() has been invoked.

Definition at line 164 of file AthMessaging.h.

{
  MsgStream* ms = m_msg_tls.get();
  if (!ms) {
    if (!m_initialized.test_and_set()) initMessaging();
    ms = new MsgStream(m_imsg,m_nm);
    m_msg_tls.reset( ms );
  }
 
  ms->setLevel (m_lvl);
  return *ms;
}

msg() [2/2]

MsgStream & AthMessaging::msg ( const MSG::Level  lvl ) const

inlineinherited

The standard message stream.

Returns a reference to the default message stream May not be invoked before sysInitialize() has been invoked.

Definition at line 179 of file AthMessaging.h.

{ return msg() << lvl; }

msgLvl()

bool AthMessaging::msgLvl ( const MSG::Level  lvl ) const

inlineinherited

Test the output level.

Parameters

lvl	The message level to test against

Returns

boolean Indicating if messages at given level will be printed

Return values

true	Messages at level "lvl" will be printed

Definition at line 151 of file AthMessaging.h.

{
  if (!m_initialized.test_and_set()) initMessaging();
  if (m_lvl <= lvl) {
    msg() << lvl;
    return true;
  } else {
    return false;
  }
}

operator=()

TRTProcessingOfStraw& TRTProcessingOfStraw::operator= ( const TRTProcessingOfStraw &  )

private

ProcessStraw()

void TRTProcessingOfStraw::ProcessStraw	(	MagField::AtlasFieldCache &	fieldCache,
		hitCollConstIter	i,
		hitCollConstIter	e,
		TRTDigit &	outdigit,
		bool &	m_alreadyPrintedPDGcodeWarning,
		double	m_cosmicEventPhase,
		int	strawGasType,
		bool	emulationArflag,
		bool	emulationKrflag,
		CLHEP::HepRandomEngine *	rndmEngine,
		CLHEP::HepRandomEngine *	elecProcRndmEngine,
		CLHEP::HepRandomEngine *	elecNoiseRndmEngine,
		CLHEP::HepRandomEngine *	paiRndmEngine
	)

Process this straw all the way from Geant4 hit to output digit.

Steps:

1. Loop over the simhits in this straw and produce a list of primary ionisation clusters.
2. Use the cluster list along with gas and wire properties, to create a list of energy deposits (i.e. potential fluctuations) reaching the frontend electronics.
3. Simulate how the FE turns the results into an output digit. This includes the shaping/amplification and subsequent discrimination as well as addition of noise.

Parameters

i	Geant4 hit collection iterator
e	last hit in collection
outdigit	The 27 bit digit (bits: 8 low + 1 high + 8 low + 1 high + 8 low + 1 high)

Definition at line 250 of file TRTProcessingOfStraw.cxx.

{
 
  // We need the straw id several times in the following  //
  const int hitID((*i)->GetHitID());
  unsigned int region(TRTDigiHelper::getRegion(hitID));
  const bool isBarrel(region<3 );
  //const bool isEC    (!isBarrel);
  //const bool isShort (region==1);
  //const bool isLong  (region==2);
  const bool isECA   (region==3);
  const bool isECB   (region==4);
 
  //======================================================//
  // First step is to loop over the simhits in this straw //
  // and produce a list of primary ionisation clusters.   //
  // Each cluster needs the following information:        //
  //                                                      //
  //  * The total energy of the cluster.                  //
  //  * Its location in local straw (x,y,z) coordinates.  //
  //  * The time the cluster was created.                 //
  //                                                      //
  //======================================================//
  // TimeShift is the same for all the simhits in the straw.
  const double timeShift(m_pTimeCorrection->TimeShift(hitID)); // rename hitID to strawID
 
  m_clusterlist.clear();
 
  //For magnetic field evaluation
  Amg::Vector3D TRThitGlobalPos(0.0,0.0,0.0);
 
  //Now we loop over all the simhits
  for (hitCollConstIter hit_iter= i;  hit_iter != e; ++hit_iter)
    {
      //Get the hit:
      const TimedHitPtr<TRTUncompressedHit> *theHit = &(*hit_iter);
 
      TRThitGlobalPos = getGlobalPosition(hitID, theHit);
 
      //Figure out the global time of the hit (all clusters from the hit
      //will get same timing).
 
      double timeOfHit(0.0); // remains zero if timeCorrection is false (beamType='cosmics')
      if (m_timeCorrection) {
        const double globalHitTime(hitTime(*theHit));
        const double globalTime = static_cast<double>((*theHit)->GetGlobalTime());
        const double bunchCrossingTime(globalHitTime - globalTime);
        if ( (bunchCrossingTime < m_minCrossingTime) || (bunchCrossingTime > m_maxCrossingTime) ) continue;
        timeOfHit = m_shiftOfZeroPoint + globalHitTime - timeShift; //is this shiftofzeropoint correct pileup-wise?? [fixme]
      }
 
      //if (timeOfHit>125.0) continue; // Will give 3% speed up (but changes seeds!). Needs careful thought though.
 
      //What kind of particle are we dealing with?
      const int particleEncoding((*theHit)->GetParticleEncoding());
 
      //Safeguard against pdgcode 0.
      if (particleEncoding == 0)
        {
          //According to Andrea this is usually nuclear fragments from
          //hadronic interactions. They therefore ought to be allowed to
          //contribute, but we ignore them for now - until it can be studied
          //that it is indeed safe to stop doing so
          if (!m_alreadywarnedagainstpdg0) {
            m_alreadywarnedagainstpdg0 = true;
            ATH_MSG_WARNING ( "Ignoring sim. particle with pdgcode 0. This warning is only shown once per job" );
          }
          continue;
        }
 
      // If it is a photon we assume it was absorbed entirely at the point of interaction.
      // we simply deposit the entire energy into the last point of the sim. step.
      if ( MC::isPhoton(particleEncoding) ) {
 
        const double energyDeposit = (*theHit)->GetEnergyDeposit(); // keV (see comment below)
        // Apply radiator efficiency "fudge factor" to ignore some TR photons (assuming they are over produced in the sim. step.
        // The fraction removed is based on tuning pHT for electrons to data, after tuning pHT for muons (which do not produce TR).
        // The efficiency is different for Xe, Kr and Ar. Avoid fudging non-TR photons (TR is < 30 keV).
        // Also: for |eta|<0.5 apply parabolic scale; see "Parabolic Fudge" https://indico.cern.ch/event/304066/
 
        if ( energyDeposit<30.0 ) {
 
          // Improved Argon Emulation tuning October 2018 by Hassane Hamdaoui https://cds.cern.ch/record/2643784
          // Previously 0.15, 0.28, 0.28
          double ArEmulationScaling_BA  = 0.05;
          double ArEmulationScaling_ECA = 0.20;
          double ArEmulationScaling_ECB = 0.20;
 
          // ROUGH GUESSES RIGHT NOW
          double KrEmulationScaling_BA = 0.20;
          double KrEmulationScaling_ECA = 0.39;
          double KrEmulationScaling_ECB = 0.39;
 
          if (isBarrel) { // Barrel
            double trEfficiencyBarrel = m_settings->trEfficiencyBarrel(strawGasType);
            double hitx = TRThitGlobalPos[0];
            double hity = TRThitGlobalPos[1];
            double hitz = TRThitGlobalPos[2];
            double hitEta = std::abs(log(tan(0.5*atan2(sqrt(hitx*hitx+hity*hity),hitz))));
            if ( hitEta < 0.5 ) { trEfficiencyBarrel *= ( 0.833333+0.6666667*hitEta*hitEta ); }
            // scale down the TR efficiency if we are emulating
            if ( strawGasType == 0 && emulationArflag ) { trEfficiencyBarrel *= ArEmulationScaling_BA; }
            if ( strawGasType == 0 && emulationKrflag ) { trEfficiencyBarrel *= KrEmulationScaling_BA; }
            if ( CLHEP::RandFlat::shoot(rndmEngine) > trEfficiencyBarrel ) continue; // Skip this photon
          } // close if barrel
          else { // Endcap - no eta dependence here.
            if (isECA) {
              double trEfficiencyEndCapA = m_settings->trEfficiencyEndCapA(strawGasType);
              // scale down the TR efficiency if we are emulating
              if ( strawGasType == 0 && emulationArflag ) { trEfficiencyEndCapA *= ArEmulationScaling_ECA; }
              if ( strawGasType == 0 && emulationKrflag ) { trEfficiencyEndCapA *= KrEmulationScaling_ECA; }
              if ( CLHEP::RandFlat::shoot(rndmEngine) > trEfficiencyEndCapA ) continue; // Skip this photon
            }
            if (isECB) {
              double trEfficiencyEndCapB = m_settings->trEfficiencyEndCapB(strawGasType);
              // scale down the TR efficiency if we are emulating
              if ( strawGasType == 0 && emulationArflag ) { trEfficiencyEndCapB *= ArEmulationScaling_ECB; }
              if ( strawGasType == 0 && emulationKrflag ) { trEfficiencyEndCapB *= KrEmulationScaling_ECB; }
              if ( CLHEP::RandFlat::shoot(rndmEngine) > trEfficiencyEndCapB ) continue; // Skip this photon
            }
          } // close else (end caps)
        } // energyDeposit < 30.0
 
          // Append this (usually highly energetic) cluster to the list:
        m_clusterlist.emplace_back( energyDeposit*CLHEP::keV, timeOfHit, (*theHit)->GetPostStepX(), (*theHit)->GetPostStepY(), (*theHit)->GetPostStepZ() );
 
        // Regarding the CLHEP::keV above: In TRT_G4_SD we converting the hits to keV,
        // so here we convert them back to CLHEP units by multiplying by CLHEP::keV.
      }
      else if ( MC::isMonopole(particleEncoding)
                || ( MC::isGenericMultichargedParticle(particleEncoding) && MC::charge(particleEncoding) > 10. )
                ) {
        //Special treatment of magnetic monopoles && highly charged Qballs (charge > 10)
        m_clusterlist.emplace_back( (*theHit)->GetEnergyDeposit()*CLHEP::keV, timeOfHit, (*theHit)->GetPostStepX(), (*theHit)->GetPostStepY(), (*theHit)->GetPostStepZ() );
      }
      else { // It's not a photon, monopole or Qball with charge > 10, so we proceed with regular ionization using the PAI model
 
        // Lookup mass and charge from the PDG info in CLHEP HepPDT:
        const HepPDT::ParticleData *particle(m_pParticleTable->particle(HepPDT::ParticleID(abs(particleEncoding))));
        double particleCharge(0.);
        double particleMass(0.);
 
        if (particle) {
          particleCharge = particle->charge();
          particleMass = particle->mass().value();
          // Override ParticleData charge value for Qballs and similar exotic multi-charged particles
          if (MC::isGenericMultichargedParticle(particleEncoding)) {
            particleCharge =MC::charge(particleEncoding);
          }
        }
        else {
          // TODO Should we handle charged Geantinos gracefully here?
          if (!MC::isNucleus(particleEncoding)) {
            ATH_MSG_WARNING ( "Data for sim. particle with pdgcode "<<particleEncoding
                              <<"  is not a nucleus and could not be retrieved from PartPropSvc. Assuming mass and charge as pion. Please investigate." );
            particleCharge = 1.;
            particleMass = ParticleConstants::chargedPionMassInMeV;
          }
          else {
            particleCharge = MC::charge(particleEncoding);
 
            const int A(static_cast<int>(MC::baryonNumber(particleEncoding)));
            const int Z(static_cast<int>(std::abs(MC::numberOfProtons(particleEncoding))));
            static constexpr double Mp(ParticleConstants::protonMassInMeV);
            static constexpr double Mn(ParticleConstants::neutronMassInMeV);
            particleMass = std::abs( Z*Mp+(A-Z)*Mn );
 
            if (!alreadyPrintedPDGcodeWarning) {
              ATH_MSG_WARNING ( "Data for sim. particle with pdgcode "<<particleEncoding
                                <<" could not be retrieved from PartPropSvc (unexpected ion)."
                                <<" Please Investigate the PDGTABLE.MeV file."
                                <<" Calculating mass and charge from pdg code."
                                <<" The result is: Charge = "<<particleCharge<<" Mass = "<<particleMass<<"MeV" );
              alreadyPrintedPDGcodeWarning = true;
            }
          }
        }
        // Abort if uncharged particle.
        if (!particleCharge) { continue; }
        // Abort if weird massless charged particle.
        if (!particleMass) {
          ATH_MSG_WARNING ( "Ignoring ionization from particle with pdg code "<<particleEncoding
                            <<" since it appears to be a massless charged particle. Please investigate." );
          continue;
        }
 
        //We are now in the most likely case: A normal ionizing
        //particle. Using the PAI model we are going to distribute
        //ionization clusters along the step taken by the sim particle.
 
        const double scaledKineticEnergy( static_cast<double>((*theHit)->GetKineticEnergy()) * ( CLHEP::proton_mass_c2 / particleMass ));
 
        addClustersFromStep ( scaledKineticEnergy, particleCharge, timeOfHit,
                              (*theHit)->GetPreStepX(),(*theHit)->GetPreStepY(),(*theHit)->GetPreStepZ(),
                              (*theHit)->GetPostStepX(),(*theHit)->GetPostStepY(),(*theHit)->GetPostStepZ(),
                              m_clusterlist, strawGasType, rndmEngine, paiRndmEngine);
 
      }
    }//end of hit loop
 
  //======================================================//
  // Second step is, using the cluster list along with    //
  // gas and wire properties, to create a list of energy  //
  // deposits (i.e. potential fluctuations) reaching the  //
  // frontend electronics. Each deposit needs:            //
  //                                                      //
  //  * The energy of the deposit.                        //
  //  * The time it arrives at the FE electronics         //
  //                                                      //
  //======================================================//
 
  m_depositList.clear();
 
  ClustersToDeposits(fieldCache, hitID, m_clusterlist, m_depositList, TRThitGlobalPos, cosmicEventPhase, strawGasType, rndmEngine );
 
 
  //======================================================//
  // The third and final step is to simulate how the FE   //
  // turns the results into an output digit. This         //
  // includes the shaping/amplification and subsequent    //
  // discrimination as well as addition of noise.         //
  //                                                      //
  //======================================================//
 
  //If no deposits, and no electronics noise we might as well stop here:
  if ( m_depositList.empty() && !m_pNoise )
    {
      outdigit = TRTDigit(hitID, 0);
      return;
    }
 
  //Get straw conditions data:
  double lowthreshold, noiseamplitude;
  if (m_settings->noiseInSimhits()) {
    m_pDigConditions->getStrawData( hitID, lowthreshold, noiseamplitude );
  } else {
    lowthreshold = isBarrel ? m_settings->lowThresholdBar(strawGasType) : m_settings->lowThresholdEC(strawGasType);
    noiseamplitude = 0.0;
  }
 
  //Electronics processing:
  m_pElectronicsProcessing->ProcessDeposits( m_depositList, hitID, outdigit, lowthreshold, noiseamplitude, strawGasType, elecProcRndmEngine, elecNoiseRndmEngine );
}

setClusterZ()

double TRTProcessingOfStraw::setClusterZ ( double  cluster_z_in, bool  isLong, bool  isShort, bool  isEC  ) const

private

Definition at line 788 of file TRTProcessingOfStraw.cxx.

                                                                                                        {
  double cluster_z(cluster_z_in);
 
  // The active gas volume along the straw z-axis is: Barrel long +-349.315 mm; Barrel short +-153.375 mm; End caps +-177.150 mm.
  // Here we give a warning for clusters that are outside of the straw gas volume in in z. Since T/P version 3 cluster z values
  // can go several mm outside these ranges; 30 mm is plenty allowance in the checks below.
  const double  longBarrelStrawHalfLength(349.315*CLHEP::mm);
  const double shortBarrelStrawHalfLength(153.375*CLHEP::mm);
  const double      EndcapStrawHalfLength(177.150*CLHEP::mm);
  if ( isLong  && std::abs(cluster_z)>longBarrelStrawHalfLength+30 ) {
    double d = cluster_z<0 ? cluster_z+longBarrelStrawHalfLength : cluster_z-longBarrelStrawHalfLength;
    ATH_MSG_WARNING ("Long barrel straw cluster is outside the active gas volume z = +- 349.315 mm by " << d << " mm.");
    ATH_MSG_WARNING ("Setting cluster_z = 0.0");
    cluster_z = 0.0;
  }
  if ( isShort && std::abs(cluster_z)>shortBarrelStrawHalfLength+30 ) {
    double d = cluster_z<0 ? cluster_z+shortBarrelStrawHalfLength : cluster_z-shortBarrelStrawHalfLength;
    ATH_MSG_WARNING ("Short barrel straw cluster is outside the active gas volume z = +- 153.375 mm by " << d << " mm.");
    ATH_MSG_WARNING ("Setting cluster_z = 0.0");
    cluster_z = 0.0;
  }
  if ( isEC    && std::abs(cluster_z)>EndcapStrawHalfLength+30 ) {
    double d = cluster_z<0 ? cluster_z+EndcapStrawHalfLength : cluster_z-EndcapStrawHalfLength;
    ATH_MSG_WARNING ("End cap straw cluster is outside the active gas volume z = +- 177.150 mm by " << d << " mm.");
    ATH_MSG_WARNING ("Setting cluster_z = 0.0");
    cluster_z = 0.0;
  }
  return cluster_z;
}

setLevel()

void AthMessaging::setLevel ( MSG::Level  lvl )

inherited

Change the current logging level.

Use this rather than msg().setLevel() for proper operation with MT.

Definition at line 28 of file AthMessaging.cxx.

{
  m_lvl = lvl;
}

Member Data Documentation

ATLAS_THREAD_SAFE

std::atomic_flag m_initialized AthMessaging::ATLAS_THREAD_SAFE = ATOMIC_FLAG_INIT

mutableprivateinherited

Messaging initialized (initMessaging)

Definition at line 141 of file AthMessaging.h.

m_alreadywarnedagainstpdg0

bool TRTProcessingOfStraw::m_alreadywarnedagainstpdg0

private

Definition at line 228 of file TRTProcessingOfStraw.h.

m_attenuationLength

double TRTProcessingOfStraw::m_attenuationLength = 0.0

private

Definition at line 128 of file TRTProcessingOfStraw.h.

m_clusterlist

std::vector<cluster> TRTProcessingOfStraw::m_clusterlist

private

Definition at line 162 of file TRTProcessingOfStraw.h.

m_depositList

std::vector<TRTElectronicsProcessing::Deposit> TRTProcessingOfStraw::m_depositList

private

Definition at line 163 of file TRTProcessingOfStraw.h.

m_detmgr

const InDetDD::TRT_DetectorManager* TRTProcessingOfStraw::m_detmgr

private

Definition at line 118 of file TRTProcessingOfStraw.h.

m_drifttimes

std::vector<double> TRTProcessingOfStraw::m_drifttimes

private

Definition at line 224 of file TRTProcessingOfStraw.h.

m_expattenuation

std::vector<double> TRTProcessingOfStraw::m_expattenuation

private

Definition at line 225 of file TRTProcessingOfStraw.h.

m_id_helper

const TRT_ID* TRTProcessingOfStraw::m_id_helper

protected

Definition at line 237 of file TRTProcessingOfStraw.h.

m_imsg

std::atomic<IMessageSvc*> AthMessaging::m_imsg { nullptr }

mutableprivateinherited

MessageSvc pointer.

Definition at line 135 of file AthMessaging.h.

m_innerRadiusOfStraw

double TRTProcessingOfStraw::m_innerRadiusOfStraw = 0.0

private

Definition at line 137 of file TRTProcessingOfStraw.h.

m_lvl

std::atomic<MSG::Level> AthMessaging::m_lvl { MSG::NIL }

mutableprivateinherited

Current logging level.

Definition at line 138 of file AthMessaging.h.

m_maxCrossingTime

double TRTProcessingOfStraw::m_maxCrossingTime = 0.0

private

Definition at line 133 of file TRTProcessingOfStraw.h.

m_maxelectrons

unsigned int TRTProcessingOfStraw::m_maxelectrons = 0U

private

Definition at line 226 of file TRTProcessingOfStraw.h.

m_minCrossingTime

double TRTProcessingOfStraw::m_minCrossingTime = 0.0

private

Definition at line 134 of file TRTProcessingOfStraw.h.

m_msg_tls

boost::thread_specific_ptr<MsgStream> AthMessaging::m_msg_tls

mutableprivateinherited

MsgStream instance (a std::cout like with print-out levels)

Definition at line 132 of file AthMessaging.h.

m_nm

std::string AthMessaging::m_nm

privateinherited

Message source name.

Definition at line 129 of file AthMessaging.h.

m_outerRadiusOfWire

double TRTProcessingOfStraw::m_outerRadiusOfWire = 0.0

private

Definition at line 138 of file TRTProcessingOfStraw.h.

m_pDigConditions

TRTDigCondBase* TRTProcessingOfStraw::m_pDigConditions

private

Definition at line 146 of file TRTProcessingOfStraw.h.

m_pElectronicsProcessing

TRTElectronicsProcessing* TRTProcessingOfStraw::m_pElectronicsProcessing

private

Definition at line 144 of file TRTProcessingOfStraw.h.

m_pNoise

TRTNoise* TRTProcessingOfStraw::m_pNoise

private

Definition at line 145 of file TRTProcessingOfStraw.h.

m_pPAItoolAr

ITRT_PAITool* TRTProcessingOfStraw::m_pPAItoolAr

private

Definition at line 120 of file TRTProcessingOfStraw.h.

m_pPAItoolKr

ITRT_PAITool* TRTProcessingOfStraw::m_pPAItoolKr

private

Definition at line 121 of file TRTProcessingOfStraw.h.

m_pPAItoolXe

ITRT_PAITool* TRTProcessingOfStraw::m_pPAItoolXe

private

Definition at line 119 of file TRTProcessingOfStraw.h.

m_pParticleTable

const HepPDT::ParticleDataTable* TRTProcessingOfStraw::m_pParticleTable

private

Definition at line 148 of file TRTProcessingOfStraw.h.

m_pSimDriftTimeTool

ITRT_SimDriftTimeTool* TRTProcessingOfStraw::m_pSimDriftTimeTool

private

Definition at line 122 of file TRTProcessingOfStraw.h.

m_pTimeCorrection

TRTTimeCorrection* TRTProcessingOfStraw::m_pTimeCorrection

private

Definition at line 143 of file TRTProcessingOfStraw.h.

m_randBinomialAr

std::unique_ptr<CLHEP::RandBinomialFixedP> TRTProcessingOfStraw::m_randBinomialAr {}

private

Definition at line 234 of file TRTProcessingOfStraw.h.

m_randBinomialKr

std::unique_ptr<CLHEP::RandBinomialFixedP> TRTProcessingOfStraw::m_randBinomialKr {}

private

Definition at line 233 of file TRTProcessingOfStraw.h.

m_randBinomialXe

std::unique_ptr<CLHEP::RandBinomialFixedP> TRTProcessingOfStraw::m_randBinomialXe {}

private

Definition at line 232 of file TRTProcessingOfStraw.h.

m_settings

const TRTDigSettings* TRTProcessingOfStraw::m_settings

private

Definition at line 117 of file TRTProcessingOfStraw.h.

m_shiftOfZeroPoint

double TRTProcessingOfStraw::m_shiftOfZeroPoint = 0.0

private

Definition at line 135 of file TRTProcessingOfStraw.h.

m_signalPropagationSpeed

double TRTProcessingOfStraw::m_signalPropagationSpeed = 0.0

private

Definition at line 127 of file TRTProcessingOfStraw.h.

m_solenoidFieldStrength

double TRTProcessingOfStraw::m_solenoidFieldStrength = 0.0

private

Definition at line 140 of file TRTProcessingOfStraw.h.

m_timeCorrection

bool TRTProcessingOfStraw::m_timeCorrection = false

private

Time to be corrected for flight and wire propagation delays false when beamType='cosmics'.

Definition at line 125 of file TRTProcessingOfStraw.h.

m_useAttenuation

bool TRTProcessingOfStraw::m_useAttenuation = false

private

Definition at line 130 of file TRTProcessingOfStraw.h.

m_useMagneticFieldMap

bool TRTProcessingOfStraw::m_useMagneticFieldMap = false

private

Definition at line 131 of file TRTProcessingOfStraw.h.

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The documentation for this class was generated from the following files:

• TRTProcessingOfStraw.h
• TRTProcessingOfStraw.cxx