2011 jinr, dubna student practice. vaclav kosar czech technical university in prague viktor burian...

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2011 JINR, DUBNA Student Practice

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Page 1: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

2011

JINR, DUBNAStudent Practice

Page 2: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

Vaclav Kosar Czech Technical University in Prague

Viktor Burian Czech Technical University in Prague

Andra-Georgia Ibanescu University of Bucharest

Page 3: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

Igor Rufanov

Elena Kokoulina

Vladimir Nikitin

Page 4: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

To understand photon production and it’s importance for collective phenomena explanations.

To get familiar with GEANT, PYTHIA, PAW To simulate the spectra of photons

produced in high energy collisions To understand how a electromagnetic

calorimeter works. To simulate the energy deposition

spectra of photons in a calorimeter.

Page 5: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 6: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

Isotropical with energy distribution:

Page 7: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 8: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

- capability to measure low energy

deposit Emin < 5MeV

- the dimension of one cell

4 x 4 x 120 cm3

- localization of photon σ < 2 cm.

Page 9: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

Red - BGO crystals

Blue - organic scintillator - cutting the charged particles Green - Veto - energy leakagesFrom GEANT

Page 10: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 11: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 12: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

50 GeV

Page 13: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 14: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

In spite of small dimension of detector it allows one to detect low energy photons with small background contribution from high energy particles.

This is achieved due to VETO detector and measurement of location of incoming photons.

Signal of soft photons is detectable for cross section of several mb, according to the simulation.

Page 15: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia
Page 16: 2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia

Generate total momentum of photons in CMS

Generate the direction of photons in CMS

Calculate the photons momentum in LS

Calculate energy of photons in LS

)/)0(exp(0 Arandpp

)5.0)0((*2,, randzyx 222 zyxr rxppCMS /*

)2,1()2,1( CMSLS pp )**

()3( pvr

zpp CMSLS

)3()2()1( 222

LSLSLSpppELS