dc/db5/SmearTrackingPreview__0__2__B3T_8cxx_source.html

// Based on

// https://physdiv.jlab.org/DetectorMatrix/

// Using everything from v 0.1 from June 16 2020 except:

// - EMCal coverage reduced to |eta|<3.5

// - Tracking parameters from B=3T Matrix preview at

//   https://indico.bnl.gov/event/9984/contributions/43066/attachments/31173/49186/YR_Detector_Matrix_Tracking_only_10282020.xlsx


// Reminder:

// Acceptance::Zone(double theta = 0., double = TMath::Pi(),

//      double phi = 0., double = TMath::TwoPi(),

//      double E = 0., double = TMath::Infinity(),

//      double p = 0., double = TMath::Infinity(),

//      double pt = 0., double = TMath::Infinity(),

//      double pz = -TMath::Infinity(), double = TMath::Infinity());


#include "eicsmear/erhic/VirtualParticle.h"

#include "eicsmear/smear/Acceptance.h"

#include "eicsmear/smear/Device.h"

#include "eicsmear/smear/Detector.h"

#include "eicsmear/smear/Smearer.h"

#include "eicsmear/smear/ParticleMCS.h"

#include "eicsmear/smear/PerfectID.h"

#include <eicsmear/smear/Smear.h>

#include <eicsmear/erhic/ParticleMC.h>

#include "Math/Vector4D.h"


// declare static --> local to this file, won't clash with others

static double ThetaFromEta( const double eta );


Smear::Detector BuildTrackingPreview_0_2_B3T() {

  gSystem->Load("libeicsmear");


  // Create the detector object to hold all devices

  Smear::Detector det;


  // The framework provides implementations of three kinematic calculation methods

  // from smeared values

  // NM - "Null method" uses the scattered lepton.

  // DA - Double Angle method

  // JB - Jacquet-Blondel method

  // Important Notes:

  // - All methods rely on measured energy and momentum components (lepton for NM, hadrons for DA, JB).

  //   In order to rely on these methods, you therefore _need_ to cover the relevant

  //   regions with smearers for momentum, angles and energy.

  // - This is exacerbated by the fact that in the current implementation a smearing of e.g. P

  //   may fool the framework into assuming theta is measured to be the initialization value 0,

  //   leading to nan or inf or otherwise wrong calculations.

  //   NM catches P=0 and replaces it in calculations with E,

  //   but JB and DA either don't work at all or report nonsenical values.

  // - It may be advantageous to use a P measurement in place of E in a more general case.

  //   In the future, we plan to change to a weighted mean approach.

  // The summary of the above is that the user should be mindful of the limitations and assumptions in

  // the calculation of smeared kinematics. Sophisticated calculations are best redone in user code

  // from the smeared particles directly.

  det.SetEventKinematicsCalculator("NM DA JB");


  // Perfect phi and theta for all particles

  // ---------------------------------------

  // TODO: Better options?

  // total coverage of the handbook for tracker, ecal, and hcal is -3.5 < eta < 3.5

  // muons no longer need special treatment! They are part of kAll

  Smear::Acceptance::Zone AngleZoneCommon(ThetaFromEta ( 3.5 ),ThetaFromEta ( -3.5 ));

  Smear::Device SmearThetaCommon(Smear::kTheta, "0.0");

  SmearThetaCommon.Accept.AddZone(AngleZoneCommon);

  SmearThetaCommon.Accept.SetGenre(Smear::kAll);

  det.AddDevice(SmearThetaCommon);


  Smear::Device SmearPhiCommon(Smear::kPhi, "0.0");

  SmearPhiCommon.Accept.AddZone(AngleZoneCommon);

  SmearPhiCommon.Accept.SetGenre(Smear::kAll);

  det.AddDevice(SmearPhiCommon);


  // Tracking  (B = 3 T)

  // --------

  // Note: Smear::kCharged checks pdg charge, so includes muons (good)

  // eta = -3.5 --  -2.5

  // sigma_p/p ~ 0.1% p + 2%

  Smear::Acceptance::Zone TrackBack1Zone(ThetaFromEta ( -2.5 ),ThetaFromEta ( -3.5 ));

  Smear::Device TrackBack1P(Smear::kP, "sqrt( pow ( 0.001*P*P, 2) + pow ( 0.02*P, 2) )");

  TrackBack1P.Accept.AddZone(TrackBack1Zone);

  TrackBack1P.Accept.SetCharge(Smear::kCharged);

  det.AddDevice(TrackBack1P);


  // eta = -2.5 --  -1

  // sigma_p/p ~ 0.02% p + 1%

  Smear::Acceptance::Zone TrackBack2Zone(ThetaFromEta ( -1 ),ThetaFromEta ( -2.5 ));

  Smear::Device TrackBack2P(Smear::kP, "sqrt( pow ( 0.0002*P*P, 2) + pow ( 0.01*P, 2) )");

  TrackBack2P.Accept.AddZone(TrackBack2Zone);

  TrackBack2P.Accept.SetCharge(Smear::kCharged);

  det.AddDevice(TrackBack2P);


  // TODO: What to make of this?

  // "200 MeV/c with 50% acceptance (similar for pi and K)"

  // Add efficiency?

  // eta = -1 -- +1

  // sigma_p/p ~ 0.02% p + 0.05%

  Smear::Acceptance::Zone TrackBarrelZone(ThetaFromEta ( 1 ),ThetaFromEta ( -1 ));

  Smear::Device TrackBarrelP(Smear::kP, "sqrt( pow ( 0.0002*P*P, 2) + pow ( 0.005*P, 2) )");

  TrackBarrelP.Accept.AddZone(TrackBarrelZone);

  TrackBarrelP.Accept.SetCharge(Smear::kCharged);

  det.AddDevice(TrackBarrelP);


  // eta = 1 -- 2.5

  // sigma_p/p ~ 0.02% p+1%

  Smear::Acceptance::Zone TrackFwd2Zone(ThetaFromEta ( 2.5 ),ThetaFromEta ( 1 ));

  Smear::Device TrackFwd2P(Smear::kP, "sqrt( pow ( 0.0002*P*P, 2) + pow ( 0.01*P, 2) )");

  TrackFwd2P.Accept.AddZone(TrackFwd2Zone);

  TrackFwd2P.Accept.SetCharge(Smear::kCharged);

  det.AddDevice(TrackFwd2P);


  // eta = 2.5 -- 3.5

  // sigma_p/p ~ 0.1% p+2%

  Smear::Acceptance::Zone TrackFwd1Zone(ThetaFromEta ( 3.5 ),ThetaFromEta ( 2.5 ));

  Smear::Device TrackFwd1P(Smear::kP, "sqrt( pow ( 0.001*P*P, 2) + pow ( 0.02*P, 2) )");

  TrackFwd1P.Accept.AddZone(TrackFwd1Zone);

  TrackFwd1P.Accept.SetCharge(Smear::kCharged);

  det.AddDevice(TrackFwd1P);


  // EM Calorimeters

  // ---------------

  // Note: Smear::kElectromagnetic == gamma + e. Does not include muons (good)


  // Calorimeter resolution usually given as sigma_E/E = const% + stocastic%/Sqrt{E}

  // EIC Smear needs absolute sigma: sigma_E = Sqrt{const*const*E*E + stoc*stoc*E}


  // Back

  // eta = -3.5 -- -2

  // stoch. = 2%

  Smear::Acceptance::Zone EmcalBackZone(ThetaFromEta ( -2 ),ThetaFromEta ( -3.5 ));

  Smear::Device EmcalBack(Smear::kE, "sqrt( pow ( 0.0*E,2 ) + pow( 0.02,2)*E)");

  EmcalBack.Accept.AddZone(EmcalBackZone);

  EmcalBack.Accept.SetGenre(Smear::kElectromagnetic);

  det.AddDevice(EmcalBack);


  // MidBack

  // eta = -2 -- -1

  // stoch. = 7%

  Smear::Acceptance::Zone EmcalMidBackZone(ThetaFromEta ( -1 ),ThetaFromEta ( -2 ));

  Smear::Device EmcalMidBack(Smear::kE, "sqrt( pow ( 0.0*E,2 ) + pow( 0.07,2)*E)");

  EmcalMidBack.Accept.AddZone(EmcalMidBackZone);

  EmcalMidBack.Accept.SetGenre(Smear::kElectromagnetic);

  det.AddDevice(EmcalMidBack);


  // Forward

  // eta = -1 -- 3.5

  // stoch. = 10-12%, use 12%

  Smear::Acceptance::Zone EmcalFwdZone(ThetaFromEta ( 3.5 ),ThetaFromEta ( -1 ));

  Smear::Device EmcalFwd(Smear::kE, "sqrt( pow ( 0.0*E,2 ) + pow( 0.12,2)*E)");

  EmcalFwd.Accept.AddZone(EmcalFwdZone);

  EmcalFwd.Accept.SetGenre(Smear::kElectromagnetic);

  det.AddDevice(EmcalFwd);


  // Could turn on perfect PID

  // Make sure to not cover more than is covered by the other detectors.

  // Using the smallest region here, but we could add a second one for

  // the extended EmCal range

  // Smear::Acceptance::Zone acceptpid(ThetaFromEta(3.5),ThetaFromEta(-3.5));

  // Smear::PerfectID pid;

  // pid.Accept.AddZone(acceptpid);

  // det.AddDevice( pid );


  // Hadronic  Calorimeters

  // ----------------------

  // Note: kHadronic == |pdg|>110.


  // Back

  // eta = -3.5 -- -1

  // stoch. = 50%

  Smear::Acceptance::Zone HcalBackZone(ThetaFromEta ( -1 ),ThetaFromEta ( -3.5 ));

  Smear::Device HcalBack(Smear::kE, "sqrt(pow( 0.0*E, 2) + pow ( 0.5,2) *E)");

  HcalBack.Accept.AddZone(HcalBackZone);

  HcalBack.Accept.SetGenre(Smear::kHadronic);

  det.AddDevice(HcalBack);


  // Barrel

  // eta = -1 -- 1

  // The matrix has nothing. As examples, one could turn to

  // ~CMS

  // Smear::Device HcalBarrel(Smear::kE, "sqrt( pow( 0.07*E, 2) + pow( 0.85, 2)*E)");

  // ~Zeus

  // Smear::Device HcalBarrel(Smear::kE, "sqrt( pow( 0.02*E, 2) + pow( 0.35,2) *E)");


  // Smear::Acceptance::Zone HcalBarrelZone(ThetaFromEta ( 1 ),ThetaFromEta ( -1 ));

  // HcalBarrel.Accept.AddZone(HcalBarrelZone);

  // HcalBarrel.Accept.SetGenre(Smear::kHadronic);

  // det.AddDevice(HcalBarrel);


  // Forward

  // eta = 1 -- 3.5

  // stoch. = 50%

  Smear::Acceptance::Zone HcalFwdZone(ThetaFromEta ( 3.5 ),ThetaFromEta ( 1 ));

  Smear::Device HcalFwd(Smear::kE, "sqrt(pow( 0.0*E, 2) + pow ( 0.5,2) *E)");

  HcalFwd.Accept.AddZone(HcalFwdZone);

  HcalFwd.Accept.SetGenre(Smear::kHadronic);

  det.AddDevice(HcalFwd);


  // Not covered:

  // Tracker material budget X/X0 <~5%

  // Low-Q^2 tagger: -6.9<eta<-5.8: Delta_theta/theta < 1.5%; 10^-6 < Q2 < 10^-2 GeV2

  // Proton spectrometer:  eta>6.2: sigma_intrinsic(|t|)/|t| < 1%; Acceptance: 0.2 < pT < 1.2 GeV/c

  // Barrel vertexing: sigma_xyz ~ 20 microns, d0(z) ~ d0(r phi) ~ (20 microns)/(pT [GeV])  + 5 microns


  return det;

}


// -------------------------------------------------------------------

double ThetaFromEta( const double eta ) {

  if ( !std::isnan(eta) && !std::isinf(eta)   ) {

    return 2.0 * atan( exp( -eta ));

  }

  throw std::runtime_error("ThetaFromEta called with NaN or Inf");

  return -1;

}