/// \file /// \ingroup tutorial_tree /// \notebook /// This example is the same as tree2.C, but uses a class instead of a C-struct. /// In this example, we are mapping a class to one of the Geant3 /// common blocks /gctrak/. In the real life, this common will be filled /// by Geant3 at each step and only the Tree Fill function should be called. /// The example emulates the Geant3 step routines. /// /// to run the example, do to execute with native compiler: /// ~~~ /// .x tree2a.C+ /// ~~~ /// /// Note that since IO is involved, ACLiC has to be invoked to create the dictionary of class Gctrak. /// \macro_code /// /// \author Rene Brun #include "TROOT.h" #include "TFile.h" #include "TTree.h" #include "TBrowser.h" #include "TH2.h" #include "TMath.h" #include "TRandom.h" #include "TCanvas.h" const Int_t MAXMEC = 30; class Gctrak : public TObject { public: Float_t vect[7]; Float_t getot; Float_t gekin; Float_t vout[7]; //! not persistent Int_t nmec; Int_t *lmec; //[nmec] Int_t *namec; //[nmec] Int_t nstep; //! not persistent Int_t pid; Float_t destep; Float_t destel; //! not persistent Float_t safety; //! not persistent Float_t sleng; //! not persistent Float_t step; //! not persistent Float_t snext; //! not persistent Float_t sfield; //! not persistent Float_t tofg; //! not persistent Float_t gekrat; //! not persistent Float_t upwght; //! not persistent Gctrak() {lmec=0; namec=0;} ClassDef(Gctrak,1) }; void helixStep(Float_t step, Float_t *vect, Float_t *vout) { // extrapolate track in constant field Float_t field = 20; //magnetic field in kilogauss enum Evect {kX,kY,kZ,kPX,kPY,kPZ,kPP}; vout[kPP] = vect[kPP]; Float_t h4 = field*2.99792e-4; Float_t rho = -h4/vect[kPP]; Float_t tet = rho*step; Float_t tsint = tet*tet/6; Float_t sintt = 1 - tsint; Float_t sint = tet*sintt; Float_t cos1t = tet/2; Float_t f1 = step*sintt; Float_t f2 = step*cos1t; Float_t f3 = step*tsint*vect[kPZ]; Float_t f4 = -tet*cos1t; Float_t f5 = sint; Float_t f6 = tet*cos1t*vect[kPZ]; vout[kX] = vect[kX] + (f1*vect[kPX] - f2*vect[kPY]); vout[kY] = vect[kY] + (f1*vect[kPY] + f2*vect[kPX]); vout[kZ] = vect[kZ] + (f1*vect[kPZ] + f3); vout[kPX] = vect[kPX] + (f4*vect[kPX] - f5*vect[kPY]); vout[kPY] = vect[kPY] + (f4*vect[kPY] + f5*vect[kPX]); vout[kPZ] = vect[kPZ] + (f4*vect[kPZ] + f6); } void tree2aw() { //create a Tree file tree2.root //create the file, the Tree and a few branches with //a subset of gctrak TFile f("tree2.root","recreate"); TTree t2("t2","a Tree with data from a fake Geant3"); Gctrak *gstep = new Gctrak; t2.Branch("track",&gstep,8000,1); //Initialize particle parameters at first point Float_t px,py,pz,p,charge=0; Float_t vout[7]; Float_t mass = 0.137; Bool_t newParticle = kTRUE; gstep->lmec = new Int_t[MAXMEC]; gstep->namec = new Int_t[MAXMEC]; gstep->step = 0.1; gstep->destep = 0; gstep->nmec = 0; gstep->pid = 0; //transport particles for (Int_t i=0;i<10000;i++) { //generate a new particle if necessary if (newParticle) { px = gRandom->Gaus(0,.02); py = gRandom->Gaus(0,.02); pz = gRandom->Gaus(0,.02); p = TMath::Sqrt(px*px+py*py+pz*pz); charge = 1; if (gRandom->Rndm() < 0.5) charge = -1; gstep->pid += 1; gstep->vect[0] = 0; gstep->vect[1] = 0; gstep->vect[2] = 0; gstep->vect[3] = px/p; gstep->vect[4] = py/p; gstep->vect[5] = pz/p; gstep->vect[6] = p*charge; gstep->getot = TMath::Sqrt(p*p + mass*mass); gstep->gekin = gstep->getot - mass; newParticle = kFALSE; } // fill the Tree with current step parameters t2.Fill(); //transport particle in magnetic field helixStep(gstep->step, gstep->vect, vout); //make one step //apply energy loss gstep->destep = gstep->step*gRandom->Gaus(0.0002,0.00001); gstep->gekin -= gstep->destep; gstep->getot = gstep->gekin + mass; gstep->vect[6] = charge*TMath::Sqrt(gstep->getot*gstep->getot - mass*mass); gstep->vect[0] = vout[0]; gstep->vect[1] = vout[1]; gstep->vect[2] = vout[2]; gstep->vect[3] = vout[3]; gstep->vect[4] = vout[4]; gstep->vect[5] = vout[5]; gstep->nmec = (Int_t)(5*gRandom->Rndm()); for (Int_t l=0;lnmec;l++) { gstep->lmec[l] = l; gstep->namec[l] = l+100; } if (gstep->gekin < 0.001) newParticle = kTRUE; if (TMath::Abs(gstep->vect[2]) > 30) newParticle = kTRUE; } //save the Tree header. The file will be automatically closed //when going out of the function scope t2.Write(); } void tree2ar() { //read the Tree generated by tree2w and fill one histogram //we are only interested by the destep branch. //note that we use "new" to create the TFile and TTree objects ! //because we want to keep these objects alive when we leave //this function. TFile *f = new TFile("tree2.root"); TTree *t2 = (TTree*)f->Get("t2"); Gctrak *gstep = 0; t2->SetBranchAddress("track",&gstep); TBranch *b_destep = t2->GetBranch("destep"); //create one histogram TH1F *hdestep = new TH1F("hdestep","destep in Mev",100,1e-5,3e-5); //read only the destep branch for all entries Long64_t nentries = t2->GetEntries(); for (Long64_t i=0;iGetEntry(i); hdestep->Fill(gstep->destep); } //we do not close the file. //We want to keep the generated histograms //We fill a 3-d scatter plot with the particle step coordinates TCanvas *c1 = new TCanvas("c1","c1",600,800); c1->SetFillColor(42); c1->Divide(1,2); c1->cd(1); hdestep->SetFillColor(45); hdestep->Fit("gaus"); c1->cd(2); gPad->SetFillColor(37); t2->SetMarkerColor(kRed); t2->Draw("vect[0]:vect[1]:vect[2]"); if (gROOT->IsBatch()) return; // invoke the x3d viewer gPad->GetViewer3D("x3d"); } void tree2a() { tree2aw(); tree2ar(); }