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He3-L derived data analysis
The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. Please consider the following formatting changes to #12220 (#12221) He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. He3-L derived data analysis The changes introduce a new data model for the LFSlimHeLambda analysis in the PWGLF module. The main changes are: 1. Add the `LFSlimHeLambda.h` file, which defines the data model for the LFHe3 and LFLambda tables. 2. Update the `he3LambdaAnalysis.cxx` file to include the new `LFSlimHeLambda.h` header file. 3. Remove the redundant code that defined the data model in the `he3LambdaAnalysis.cxx` file, as it is now provided by the `LFSlimHeLambda.h` header. These changes aim to centralize the data model definition for the LFSlimHeLambda analysis, making it more maintainable and reusable across different analysis tasks. Please consider the following formatting changes to #12220 (#12221) Please consider the following formatting changes to #12220 (#12221)
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‎PWGLF/DataModel/LFSlimHeLambda.h‎

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// Copyright 2019-2020 CERN and copyright holders of ALICE O2.
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// See https://alice-o2.web.cern.ch/copyright for details of the copyright holders.
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// All rights not expressly granted are reserved.
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//
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// This software is distributed under the terms of the GNU General Public
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// License v3 (GPL Version 3), copied verbatim in the file "COPYING".
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//
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// In applying this license CERN does not waive the privileges and immunities
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// granted to it by virtue of its status as an Intergovernmental Organization
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// or submit itself to any jurisdiction.
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///
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/// \file LFSlimNucleiTables.h
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/// \brief Slim nuclei tables
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///
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#ifndef PWGLF_DATAMODEL_LFSLIMNUCLEITABLES_H_
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#define PWGLF_DATAMODEL_LFSLIMNUCLEITABLES_H_
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#include "Framework/ASoAHelpers.h"
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#include "Framework/AnalysisDataModel.h"
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#include <Math/Vector4D.h>
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namespace o2::aod
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{
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namespace lfv0he3
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{
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DECLARE_SOA_COLUMN(Z, z, float);
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DECLARE_SOA_COLUMN(CentT0C, centT0C, float);
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} // namespace lfv0he3
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DECLARE_SOA_TABLE(LFEvents, "AOD", "LFEVENT", o2::soa::Index<>, lfv0he3::Z, lfv0he3::CentT0C);
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namespace lfv0he3
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{
36+
DECLARE_SOA_INDEX_COLUMN(LFEvent, lfEvent); // Collision ID for the event
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DECLARE_SOA_COLUMN(Pt, pt, float);
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DECLARE_SOA_COLUMN(Eta, eta, float);
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DECLARE_SOA_COLUMN(Phi, phi, float);
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DECLARE_SOA_COLUMN(Mass, mass, float);
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DECLARE_SOA_COLUMN(CosPA, cosPA, float);
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DECLARE_SOA_COLUMN(DCAxy, dcaXY, float);
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DECLARE_SOA_COLUMN(DCAz, dcaZ, float);
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DECLARE_SOA_COLUMN(TPCnCls, tpcNCls, int);
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DECLARE_SOA_COLUMN(ITSClusterSizes, itsClusterSizes, uint32_t);
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DECLARE_SOA_COLUMN(NsigmaTPC, nSigmaTPC, float);
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// DECLARE_SOA_COLUMN(NsigmaTPCproton, nSigmaTPCproton, float);
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DECLARE_SOA_COLUMN(DCAdaughters, dcaDaughters, float);
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DECLARE_SOA_COLUMN(DCAPVProton, dcaPVProton, float);
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DECLARE_SOA_COLUMN(DCAPVPion, dcaPVPion, float);
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DECLARE_SOA_COLUMN(V0Radius, v0Radius, float);
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DECLARE_SOA_COLUMN(Sign, sign, int8_t);
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} // namespace lfv0he3
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DECLARE_SOA_TABLE(LFHe3, "AOD", "LFHE3V0", lfv0he3::LFEventId, lfv0he3::Pt, lfv0he3::Eta, lfv0he3::Phi, lfv0he3::DCAxy, lfv0he3::DCAz, lfv0he3::TPCnCls, lfv0he3::ITSClusterSizes, lfv0he3::NsigmaTPC, lfv0he3::Sign);
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DECLARE_SOA_TABLE(LFLambda, "AOD", "LFLAMBDA", lfv0he3::LFEventId, lfv0he3::Pt, lfv0he3::Eta, lfv0he3::Phi, lfv0he3::Mass, lfv0he3::CosPA, lfv0he3::DCAdaughters, lfv0he3::DCAPVProton, lfv0he3::DCAPVPion, lfv0he3::V0Radius, lfv0he3::Sign);
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} // namespace o2::aod
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struct he3Candidate {
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ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>> momentum; // 4-momentum of the He3 candidate
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float nSigmaTPC = -999.f; // TPC nSigma for He3
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float dcaXY = -999.f;
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float dcaZ = -999.f;
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int tpcNClsFound = 0; // Number of TPC clusters found
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int itsNCls = 0; // Number of ITS clusters
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uint32_t itsClusterSizes = 0; // ITS cluster sizes
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int8_t sign = 0; // Charge sign of the He3 candidate
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};
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struct lambdaCandidate {
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ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>> momentum;
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float mass = -1.f; // Lambda mass
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float cosPA = -2.f; // Cosine of pointing angle
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float dcaV0Daughters = -999.f; // DCA between V0 daughters
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float dcaProtonToPV = -999.f; // DCA of the proton to primary vertex
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float dcaPionToPV = -999.f; // DCA of the pion to primary vertex
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float v0Radius = -1.f; // V0 radius
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float protonNSigmaTPC = -999.f; // Proton TPC nSigma
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float pionNSigmaTPC = -999.f;
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int8_t sign = 0; // Charge sign of the Lambda candidate
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};
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#endif // PWGLF_DATAMODEL_LFSLIMNUCLEITABLES_H_

‎PWGLF/TableProducer/Nuspex/he3LambdaAnalysis.cxx‎

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@@ -9,6 +9,8 @@
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// granted to it by virtue of its status as an Intergovernmental Organization
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// or submit itself to any jurisdiction.
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#include "PWGLF/DataModel/LFSlimHeLambda.h"
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#include "Common/Core/trackUtilities.h"
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#include "Common/DataModel/Centrality.h"
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#include "Common/DataModel/EventSelection.h"
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using namespace o2::framework;
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using namespace o2::framework::expressions;
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using namespace o2::constants::physics;
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namespace o2::aod
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{
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namespace lfv0he3
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{
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DECLARE_SOA_COLUMN(Z, z, float);
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DECLARE_SOA_COLUMN(CentT0C, centT0C, float);
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} // namespace lfv0he3
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DECLARE_SOA_TABLE(LFEvents, "AOD", "LFEVENT", o2::soa::Index<>, lfv0he3::Z, lfv0he3::CentT0C);
57-
58-
namespace lfv0he3
59-
{
60-
DECLARE_SOA_INDEX_COLUMN(LFEvent, lfEvent); // Collision ID for the event
61-
DECLARE_SOA_COLUMN(Pt, pt, float);
62-
DECLARE_SOA_COLUMN(Eta, eta, float);
63-
DECLARE_SOA_COLUMN(Phi, phi, float);
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DECLARE_SOA_COLUMN(Mass, mass, float);
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DECLARE_SOA_COLUMN(CosPA, cosPA, float);
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DECLARE_SOA_COLUMN(DCAxy, dcaXY, float);
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DECLARE_SOA_COLUMN(DCAz, dcaZ, float);
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DECLARE_SOA_COLUMN(TPCnCls, tpcNCls, int);
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DECLARE_SOA_COLUMN(ITSClusterSizes, itsClusterSizes, uint32_t);
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DECLARE_SOA_COLUMN(NsigmaTPC, nSigmaTPC, float);
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DECLARE_SOA_COLUMN(DCAdaughters, dcaDaughters, float);
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DECLARE_SOA_COLUMN(DCAPVProton, dcaPVProton, float);
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DECLARE_SOA_COLUMN(DCAPVPion, dcaPVPion, float);
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DECLARE_SOA_COLUMN(V0Radius, v0Radius, float);
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DECLARE_SOA_COLUMN(Sign, sign, int8_t);
76-
} // namespace lfv0he3
77-
DECLARE_SOA_TABLE(LFHe3, "AOD", "LFHE3V0", lfv0he3::LFEventId, lfv0he3::Pt, lfv0he3::Eta, lfv0he3::Phi, lfv0he3::DCAxy, lfv0he3::DCAz, lfv0he3::TPCnCls, lfv0he3::ITSClusterSizes, lfv0he3::NsigmaTPC, lfv0he3::Sign);
78-
DECLARE_SOA_TABLE(LFLambda, "AOD", "LFLAMBDA", lfv0he3::LFEventId, lfv0he3::Pt, lfv0he3::Eta, lfv0he3::Phi, lfv0he3::Mass, lfv0he3::CosPA, lfv0he3::DCAdaughters, lfv0he3::DCAPVProton, lfv0he3::DCAPVPion, lfv0he3::V0Radius, lfv0he3::Sign);
79-
} // namespace o2::aod
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8150
namespace
8251
{
8352
constexpr double betheBlochDefault[1][6]{{-1.e32, -1.e32, -1.e32, -1.e32, -1.e32, -1.e32}};
@@ -106,37 +75,14 @@ std::shared_ptr<TH2> hTPCnSigmaAll;
10675
std::shared_ptr<TH2> hTPCnSigmaHe3;
10776
std::shared_ptr<TH2> hArmenterosPodolanskiAll;
10877
std::shared_ptr<TH2> hArmenterosPodolanskiSelected;
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std::shared_ptr<TH2> hInvariantMass;
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std::shared_ptr<TH2> hInvariantMassUS;
79+
std::shared_ptr<TH2> hInvariantMassLS;
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11181
}; // namespace
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11383
using TracksFull = soa::Join<aod::TracksIU, aod::TracksExtra, aod::TracksCovIU, aod::pidTPCFullPr, aod::pidTPCFullPi>;
11484
using CollisionsFull = soa::Join<aod::Collisions, aod::EvSels, aod::CentFT0As, aod::CentFT0Cs, aod::CentFT0Ms>;
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116-
struct he3Candidate {
117-
ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>> momentum; // 4-momentum of the He3 candidate
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float nSigmaTPC; // TPC nSigma for He3
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float dcaXY;
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float dcaZ;
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int tpcNClsFound; // Number of TPC clusters found
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int itsNCls; // Number of ITS clusters
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uint32_t itsClusterSizes; // ITS cluster sizes
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int8_t sign; // Charge sign of the He3 candidate
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};
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struct lambdaCandidate {
128-
ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>> momentum;
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float mass; // Lambda mass
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float cosPA; // Cosine of pointing angle
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float dcaV0Daughters; // DCA between V0 daughters
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float dcaProtonToPV; // DCA of the proton to primary vertex
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float dcaPionToPV; // DCA of the pion to primary vertex
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float v0Radius;
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float protonNSigmaTPC; // Proton TPC nSigma
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float pionNSigmaTPC;
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int8_t sign; // Charge sign of the Lambda candidate
138-
};
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14086
struct he3LambdaAnalysis {
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14288
// Services
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251197
hArmenterosPodolanskiSelected = mRegistry.add<TH2>("hArmenterosPodolanskiSelected", "Armenteros-Podolanski Selected", {HistType::kTH2D, {{100, -1., 1.}, {100, 0., 0.5}}});
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253199
constexpr double ConstituentsMass = o2::constants::physics::MassProton + o2::constants::physics::MassNeutron * 2 + o2::constants::physics::MassSigmaPlus;
254-
hInvariantMass = mRegistry.add<TH2>("hInvariantMass", "Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
200+
hInvariantMassUS = mRegistry.add<TH2>("hInvariantMassUS", "Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
201+
hInvariantMassLS = mRegistry.add<TH2>("hInvariantMassLS", "Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
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256203
LOGF(info, "He3-Lambda analysis initialized");
257204
}
@@ -439,7 +386,7 @@ struct he3LambdaAnalysis {
439386
for (const auto& he3 : he3Candidates) {
440387
for (const auto& lambda : lambdaCandidates) {
441388
auto pairMomentum = lambda.momentum + he3.momentum; // Calculate invariant mass
442-
hInvariantMass->Fill(pairMomentum.Pt(), pairMomentum.M());
389+
(he3.sign * lambda.sign > 0 ? hInvariantMassLS : hInvariantMassUS)->Fill(pairMomentum.Pt(), pairMomentum.M());
443390
}
444391
}
445392
}

‎PWGLF/Tasks/Nuspex/CMakeLists.txt‎

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PUBLIC_LINK_LIBRARIES O2Physics::AnalysisCore
146146
COMPONENT_NAME Analysis)
147147

148+
o2physics_add_dpl_workflow(he3-lambda-derived-analysis
149+
SOURCES he3LambdaDerivedAnalysis.cxx
150+
PUBLIC_LINK_LIBRARIES O2Physics::AnalysisCore
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COMPONENT_NAME Analysis)
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148153
endif()

‎PWGLF/Tasks/Nuspex/he3LambdaDerivedAnalysis.cxx‎

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// Copyright 2019-2020 CERN and copyright holders of ALICE O2.
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// See https://alice-o2.web.cern.ch/copyright for details of the copyright holders.
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// All rights not expressly granted are reserved.
4+
//
5+
// This software is distributed under the terms of the GNU General Public
6+
// License v3 (GPL Version 3), copied verbatim in the file "COPYING".
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//
8+
// In applying this license CERN does not waive the privileges and immunities
9+
// granted to it by virtue of its status as an Intergovernmental Organization
10+
// or submit itself to any jurisdiction.
11+
12+
#include "PWGLF/DataModel/LFSlimHeLambda.h"
13+
14+
#include <Framework/ASoAHelpers.h>
15+
#include <Framework/AnalysisTask.h>
16+
#include <Framework/HistogramRegistry.h>
17+
#include <Framework/runDataProcessing.h>
18+
19+
#include <Math/Vector4D.h>
20+
21+
#include <memory>
22+
23+
namespace
24+
{
25+
std::shared_ptr<TH2> hInvariantMassUS[2];
26+
std::shared_ptr<TH2> hInvariantMassLS[2];
27+
std::shared_ptr<TH2> hRotationInvariantMassUS[2];
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std::shared_ptr<TH2> hRotationInvariantMassLS[2];
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std::shared_ptr<TH2> hRotationInvariantMassAntiLSeta[2];
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std::shared_ptr<TH2> hInvariantMassLambda[2];
31+
std::shared_ptr<TH2> hCosPALambda;
32+
std::shared_ptr<TH2> hNsigmaHe3;
33+
std::shared_ptr<TH2> hNsigmaProton;
34+
}; // namespace
35+
36+
using namespace o2;
37+
using namespace o2::framework;
38+
using namespace o2::framework::expressions;
39+
using namespace o2::constants::physics;
40+
41+
struct he3LambdaDerivedAnalysis {
42+
HistogramRegistry mRegistry{"He3LambdaDerivedAnalysis"};
43+
44+
Configurable<int> cfgNrotations{"cfgNrotations", 7, "Number of rotations for He3 candidates"};
45+
Configurable<bool> cfgMirrorEta{"cfgMirrorEta", true, "Mirror eta for He3 candidates"};
46+
Configurable<float> cfgMinCosPA{"cfgMinCosPA", 0.99, "Minimum cosPA for Lambda candidates"};
47+
Configurable<float> cfgMaxNSigmaTPCHe3{"cfgMaxNSigmaTPCHe3", 2.0, "Maximum nSigmaTPC for He3 candidates"};
48+
Configurable<float> cfgMinLambdaPt{"cfgMinLambdaPt", 0.4, "Minimum pT for Lambda candidates"};
49+
Configurable<float> cfgMaxLambdaDeltaM{"cfgMaxLambdaDeltaM", 10.0e-3, "Maximum deltaM for Lambda candidates"};
50+
51+
void init(InitContext const&)
52+
{
53+
constexpr double ConstituentsMass = o2::constants::physics::MassProton + o2::constants::physics::MassNeutron * 2 + o2::constants::physics::MassSigmaPlus;
54+
for (int i = 0; i < 2; ++i) {
55+
hInvariantMassUS[i] = mRegistry.add<TH2>(Form("hInvariantMassUS%i", i), "Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
56+
hInvariantMassLS[i] = mRegistry.add<TH2>(Form("hInvariantMassLS%i", i), "Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
57+
hRotationInvariantMassUS[i] = mRegistry.add<TH2>(Form("hRotationInvariantMassUS%i", i), "Rotation Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
58+
hRotationInvariantMassLS[i] = mRegistry.add<TH2>(Form("hRotationInvariantMassLS%i", i), "Rotation Invariant Mass", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
59+
hInvariantMassLambda[i] = mRegistry.add<TH2>(Form("hInvariantMassLambda%i", i), "Invariant Mass Lambda", {HistType::kTH2D, {{50, 0., 10.}, {30, o2::constants::physics::MassLambda0 - 0.015, o2::constants::physics::MassLambda0 + 0.015}}});
60+
hRotationInvariantMassAntiLSeta[i] = mRegistry.add<TH2>(Form("hRotationInvariantMassAntiLSeta%i", i), "Rotation Invariant Mass Anti-Lambda", {HistType::kTH2D, {{45, 1., 10}, {100, ConstituentsMass - 0.05, ConstituentsMass + 0.05}}});
61+
}
62+
hCosPALambda = mRegistry.add<TH2>("hCosPALambda", "Cosine of Pointing Angle for Lambda", {HistType::kTH2D, {{50, 0., 10.}, {500, 0.9, 1.}}});
63+
hNsigmaHe3 = mRegistry.add<TH2>("hNsigmaHe3", "nSigma TPC for He3", {HistType::kTH2D, {{100, -10., 10.}, {200, -5, 5.}}});
64+
hNsigmaProton = mRegistry.add<TH2>("hNsigmaProton", "nSigma TPC for Proton", {HistType::kTH2D, {{100, -10., 10.}, {200, -5, 5.}}});
65+
}
66+
67+
void processSameEvent(o2::aod::LFEvents::iterator const& collision, o2::aod::LFHe3 const& he3s, o2::aod::LFLambda const& lambdas)
68+
{
69+
std::vector<he3Candidate> he3Candidates;
70+
he3Candidates.reserve(he3s.size());
71+
std::vector<lambdaCandidate> lambdaCandidates;
72+
lambdaCandidates.reserve(lambdas.size());
73+
for (const auto& he3 : he3s) {
74+
if (he3.lfEventId() != collision.globalIndex()) {
75+
std::cout << "He3 candidate does not match event index, skipping." << std::endl;
76+
return;
77+
}
78+
he3Candidate candidate;
79+
candidate.momentum = ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>>(he3.pt(), he3.eta(), he3.phi(), o2::constants::physics::MassHelium3);
80+
candidate.nSigmaTPC = he3.nSigmaTPC();
81+
candidate.dcaXY = he3.dcaXY();
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candidate.dcaZ = he3.dcaZ();
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candidate.tpcNClsFound = he3.tpcNCls();
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candidate.itsNCls = he3.itsClusterSizes();
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candidate.itsClusterSizes = he3.itsClusterSizes();
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candidate.sign = he3.sign();
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hNsigmaHe3->Fill(he3.pt() * he3.sign(), he3.nSigmaTPC());
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if (std::abs(he3.nSigmaTPC()) > cfgMaxNSigmaTPCHe3) {
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continue; // Skip candidates with nSigmaTPC outside range
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}
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he3Candidates.push_back(candidate);
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}
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for (const auto& lambda : lambdas) {
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if (lambda.lfEventId() != collision.globalIndex()) {
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std::cout << "Lambda candidate does not match event index, skipping." << std::endl;
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return;
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}
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lambdaCandidate candidate;
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candidate.momentum.SetCoordinates(lambda.pt(), lambda.eta(), lambda.phi(), o2::constants::physics::MassLambda0);
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candidate.mass = lambda.mass();
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candidate.cosPA = lambda.cosPA();
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candidate.dcaV0Daughters = lambda.dcaDaughters();
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hCosPALambda->Fill(lambda.pt(), candidate.cosPA);
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// hNsigmaProton->Fill(lambda.pt() * lambda.sign(), lambda.protonNSigmaTPC());
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hInvariantMassLambda[0]->Fill(lambda.pt(), lambda.mass());
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if (candidate.cosPA < cfgMinCosPA || lambda.pt() < cfgMinLambdaPt ||
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std::abs(lambda.mass() - o2::constants::physics::MassLambda0) > cfgMaxLambdaDeltaM) {
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continue; // Skip candidates with low cosPA
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}
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hInvariantMassLambda[1]->Fill(lambda.pt(), lambda.mass());
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lambdaCandidates.push_back(candidate);
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}
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for (const auto& he3 : he3Candidates) {
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for (const auto& lambda : lambdaCandidates) {
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auto pairMomentum = lambda.momentum + he3.momentum; // Calculate invariant mass
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(he3.sign * lambda.sign > 0 ? hInvariantMassLS : hInvariantMassUS)[he3.sign > 0]->Fill(pairMomentum.Pt(), pairMomentum.M());
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}
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for (int iEta{0}; iEta <= cfgMirrorEta; ++iEta) {
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for (int iR{0}; iR <= cfgNrotations; ++iR) {
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auto he3Momentum = ROOT::Math::LorentzVector<ROOT::Math::PtEtaPhiM4D<double>>(he3.momentum.Pt(), (1. - iEta * 2.) * he3.momentum.Eta(), he3.momentum.Phi() + TMath::Pi() * (0.75 + 0.5 * iR / cfgNrotations), he3.momentum.M());
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for (const auto& lambda : lambdaCandidates) {
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auto pairMomentum = lambda.momentum + he3Momentum; // Calculate invariant mass
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(he3.sign * lambda.sign > 0 ? hRotationInvariantMassLS : hRotationInvariantMassUS)[he3.sign > 0]->Fill(pairMomentum.Pt(), pairMomentum.M());
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if (he3.sign < 0 && lambda.sign < 0) {
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hRotationInvariantMassAntiLSeta[iEta]->Fill(pairMomentum.Pt(), pairMomentum.M());
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}
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}
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}
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}
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}
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}
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PROCESS_SWITCH(he3LambdaDerivedAnalysis, processSameEvent, "Process same event", true);
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};
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WorkflowSpec defineDataProcessing(ConfigContext const& cfgc)
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{
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return WorkflowSpec{
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adaptAnalysisTask<he3LambdaDerivedAnalysis>(cfgc)};
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}

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