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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
parton_string
hadronization
src
G4VKinkyStringDecay.cc
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// $Id$
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// Maxim Komogorov
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//
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// -----------------------------------------------------------------------------
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// GEANT 4 class implementation file
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//
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// History: first implementation, Maxim Komogorov, 10-Oct-1998
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// -----------------------------------------------------------------------------
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#include "
G4VKinkyStringDecay.hh
"
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#include "
G4KineticTrackVector.hh
"
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#include "
G4KineticTrack.hh
"
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#include "
Randomize.hh
"
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//*****************************************************************************************************
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G4VKinkyStringDecay::G4VKinkyStringDecay
(
G4VLongitudinalStringDecay
* theModal)
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{
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this->
SetLongitudinalStringDecay
(theModal);
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}
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//*****************************************************************************************************
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G4double
G4VKinkyStringDecay::GetLightConeGluonZ
(
G4double
zmin,
G4double
zmax)
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{
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G4double
z
, yf;
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do
{
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z = zmin +
G4UniformRand
()*(zmax-zmin);
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yf = z*z +
sqr
(1 - z);
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}
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while
(
G4UniformRand
() > yf);
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return
z
;
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}
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//*****************************************************************************************************
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G4KineticTrackVector
*
G4VKinkyStringDecay::FragmentString
(
const
G4ExcitedString
& String)
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{
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G4LorentzVector
Mom = String.
GetGluon
()->
Get4Momentum
();
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G4ThreeVector
Pos
= String.
GetGluon
()->
GetPosition
();
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G4int
QuarkEncoding = theLongitudinalStringDecay->
SampleQuarkFlavor
();
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G4ThreeVector
Pquark=theLongitudinalStringDecay->
SampleQuarkPt
();
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G4double
Pt2 = Pquark.
mag2
();
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G4double
z
=
GetLightConeGluonZ
(0, 1);
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G4double
w = Mom.
e
() + Mom.
pz
();
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//... now compute quark longitudinal momentum and energy
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Pquark.
setZ
( (z*w - Pt2/(z*w))*0.5);
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G4double
E = (z*w + Pt2/(z*w))*0.5;
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G4Parton
* AntiColor =
new
G4Parton
(-QuarkEncoding);
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AntiColor->
SetPosition
(Pos);
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G4LorentzVector
AntiColorMom(-Pquark, E);
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AntiColor->
Set4Momentum
(AntiColorMom);
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G4Parton
*
Color
=
new
G4Parton
(*String.
GetColorParton
());
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G4ExcitedString
Str1(Color, AntiColor, String.
GetDirection
());
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G4KineticTrackVector
* KTV1 = theLongitudinalStringDecay->
FragmentString
(Str1);
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Color =
new
G4Parton
(QuarkEncoding);
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Color->
SetPosition
(Pos);
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G4LorentzVector
ColorMom(Pquark, E);
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Color->
Set4Momentum
(ColorMom);
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AntiColor =
new
G4Parton
(*String.
GetAntiColorParton
());
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G4ExcitedString
Str2(Color, AntiColor, String.
GetDirection
());
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G4KineticTrackVector
* KTV2 = theLongitudinalStringDecay->
FragmentString
(Str2);
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if
(KTV1 && KTV2)
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while
(!KTV2->empty())
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{
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KTV1->push_back(KTV2->back());
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KTV1->erase(KTV1->end()-1);
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}
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return
KTV1;
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}
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//*****************************************************************************************************
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