Title: Jia Shen
1Dilepton Spectra from Open Charm Decays in
Heavy-Ion Collisions
- Jia Shen
- Saint Marys College of California
- Dr. Ralf Rapp
- Cyclotron Institute at Texas AM University
2Quark-Gluon Plasma and Heavy-Ion Collisions
- A quark-gluon plasma is believed to exist during
the first 10 microseconds after the universe is
created from the Big Bang. - In the heavy-ion collision, a quark-gluon plasma
is believed to exist for a very short time.
rhic.physics.wayne.edu/sean/collision_a.gif
3Particles produced in a Heavy-Ion Collision as
seen by the STAR Detector
http//en.wikipedia.org/wiki/Quark-gluon_plasma
4This project
- How to detect the Quark-Gluon Plasma?
- Idea
- - Light quarks and gluons thermalize quickly
and lose imprinted information - - charm quarks are much heavier and do not
easily thermalize gt more sensitive probe of
interactions in QGP - - use di-electron decay spectra from charm
- quarks to probe Quark-Gluon Plasma
5Dilepton Spectra from PHENIX Collaboration (2007)
- Dileptons from charm dominant in the M1-3GeV
mass region!
6Step-1Angular Correlation between charm and
anticharm quark
- Back-to-Back
- (no interaction)
- Random angle
- (thermalization)
7Step-2 Input charm transverse-momentum
spectra dN/dPt c Pt e(-Et/Teff)
- key parameter Teff gt slope of the charm
spectrum
8Step-3Procedure to calculate ee- spectrum
- Decay c-quark into positron in its rest system
- boost positron into lab system
- repeat for anticharm -gt electron
- Calculate invariant mass of electron-positron
pair M2(E_E)2-(P_P)2 - study dependence of invariant mass distribution
on charm-quark input (slope and angular
correlation)
9Result-1 Sensitivity to charm-anticharm
relative angle
- random angle gives softer spectrum than
back-to-back (180deg)
10Result-2Sensitivity to slope of charm spectrum
Back-to-back
Random Angle
- softer charm pt-spectrum reflects itself in
softer dilepton - invariant-mass spectrum for both angular
scenarios
11Conclusions
- Sensitivity of dilepton spectra to single-charm
and charm-anticharm correlations confirmed and
quantified - Experimental acceptance cuts implemented
12- Future Directions
- More realistic charm-anticharm input spectra
- Check against single electron spectra in p-p
collisions - Use a model for charm-quark Interactions in the
QGP (consistent with single-electron spectra in
Au-Au Collisions) to obtain charm and dilepton
spectra in Au-Au collisions