Re: what a royal pain ...

From: Peter Malzacher (malzache@fnal.gov)
Date: Fri Jan 28 2000 - 23:31:13 MET


Hi Jeff,


> Pain #1 - reattaching the Tree in the ROOT file seems to be much more
> complex than hi/fil 1 charm.root was
> 
> Pain #2 - I don't see an easy way to go thru the entire Tree and plot
> say the magnitudes of the four-momenta (I thought the tree was
> supposed to keep all the object code intact which is why we were using
> C++ ... oh dear).
> 
...
> 
> ppsi.Mag() is the biggest disappointment.  What is the use of having
> all these objects in the tree if I can't use their methods?
> 
> Pain #3 - wading thru the documentation gives me no clue of how to do
> what I want to do, except for possibly the contorted, non-simple
> method shown under "The General Way" on URL
> 
>         http://root.cern.ch/root/HowtoReadTree.html
> 
> Say it ain't so!!!  Isn't OO supposed to make my life easier?
> 

I agree that it is difficult to find the way through the documentation.
But if you know how to use it its quite powerful.

I changed your macro to store objects and not numbers in the tree.
The important point is to provide the  ClassName and the address of
a pointer to the object in tree->Branch(...):

// #-> charm.py -- simulate j/psi electroproduction at JLab
// c++ version i hope

// from Numeric import *  [ left over from python version ]
// from vec4 import *
// import RNG

// #-> simulation driver parameters

void createTree(int howmany = 100)
{
  float mj = 3096.88;      //   # J/psi mass in MeV
  float me =    0.510999;  //   # electron mass
  float mp =  938.272;

  float beamen = 11.0 * 1000.0; // # GeV * 1000 MeV/GeV

  float ll_the = (3.1415926 / 180) *  1.0; // last number is e- angle LL
in deg
  float ul_the = (3.1415926 / 180) * 20.0; // last number is e- angle UL
in deg

// above is stored in radians since we will need to take cosines
// below is not

  float ll_phe = -93.0; // LL on e- azimuthal angle (degrees now)
  float ul_phe = -87.0;

  float ll_pe = 2275; // LL on scat electron momentum (MeV/c)
  float ul_pe = 2780;

// #-> set up random generators for electron.  strategy: create sample
// #-> arrays at start of program, just take values from them during
// #-> execution

  TF1 *thegen = new TF1("thegen","sin(x)",ll_the,ul_the);
  TF1 *phegen = new TF1("phegen","1.0",   ll_phe,ul_phe);
  TF1 *pegen  = new TF1("pegen", "1.0",   ll_pe, ul_pe );

  // #-> set up four-momenta for beam and target, which should not
change

  TLorentzVector *beam = new TLorentzVector();
  beam->SetVectM(TVector3(0,0,beamen),me);
  TLorentzVector *targ =new TLorentzVector(0.0,0.0,0.0,mp);

  TFile hfile("charm.root","RECREATE","Charm");

  TTree *tree = new TTree("T","Charm Electroproduction");

  int nev = 0;
  TLorentzVector *scat = new TLorentzVector(1,1,1,1);
  TLorentzVector *X = new TLorentzVector();
 
  int buf = 32000; // default in TTree
  tree->Branch("beam","TLorentzVector",&beam, buf, 0);
  tree->Branch("targ","TLorentzVector",&targ, buf, 0);
  tree->Branch("scat","TLorentzVector",&scat, buf, 0);
  tree->Branch("ppsi","TLorentzVector",&X, buf,0);

  for ( int nev = 1; nev <= howmany; nev++) {
    float thtmp = thegen.GetRandom();
    float phtmp = phegen.GetRandom();
    float ptmp  = pegen.GetRandom();

    scat->SetVectM(TVector3(ptmp*sin(thtmp)*cos(phtmp),
                           ptmp*sin(thtmp)*sin(phtmp),
                           ptmp*cos(thtmp)),
                  me);

    *X = *beam + *targ - *scat;

    tree->Fill();
  }

  hfile.Write();
  hfile.Close();
}


usage:

to create a tree:

root> .L createTree.C
root> createTree(1000)
root> .q

to use the tree:

root> TFile f("charm.root")
root> T->Draw("ppsi.X()")
root> T->Draw("ppsi.Mag()")
root> T->Draw("ppsi.X():ppsi.Y()","ppsiMag()>4000","lego")
...

If you need the full flexibility you can use
T->MakeClass("Charm")
and edit the created Charm::Loop() method.

Hope that helps,

Peter 

PS: A good starting point is the Fermi Root 102 Class
    available via http://www-pat.fnal.gov/root/


Peter Malzacher, FNAL, GSI
P.Malzacher@gsi.de



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