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Collisional energy loss in a finite size QCD medium revisited Alejandro Ayala Instituto de Ciencias Nucleares, UNAM.

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Presentation on theme: "Collisional energy loss in a finite size QCD medium revisited Alejandro Ayala Instituto de Ciencias Nucleares, UNAM."— Presentation transcript:

1 Collisional energy loss in a finite size QCD medium revisited Alejandro Ayala Instituto de Ciencias Nucleares, UNAM

2 Radiative and collisional energy losses

3 Mass and color charge effects…

4 Energy loss issues  Collisional vs radiative energy losses  Mass and color charge effects  Running of  s  Non-perturbative calculations using AdS/CFT and duality arguments ...  Finite size effects

5 A A B B Particle production region Q: How does the size of the interaction region play a role in the description of parton energy losses? Finite size effects

6 S. Peigné, P.B. Gossiaux and T. Gousset, JHEP04, 011 (2006) Energy loss computed by slowing down of parton induced by medium produced chromoelectric field in Abelian approximation Retardation effects: A fast parton produced in the medium needs to travel some distance before losing energy at the highest rate. Conclusion: finite size reduces the rate of energy loss. Conserved current

7 M. Djordjevic, PRC 74, 064907 (2006) Condition for interaction between jet and medium parton to occur inside finite QCD medium of size L. Conclusion: finite size does not affect the rate of energy loss. Perturbative collisional energy loss, 2  2 processes in a finite QCD medium Particle source

8 Scattering diagram Source: J (t, x )

9 Classical, conserved current Simple model: Color singlet dipole, i.e., two partons in color singlet state traveling with velocities v 1 and v 2 In Fourier space, this is: + (retarded prescription)

10 But suppose    ( finite) Current life-time: In Fourier space:

11 Parton should travel length of plasma Interaction rate involves ratio of currents after and without collision Explicit dependence on current life-time

12 Scattering diagram Source: J (t, x )

13 Modified matrix element Current life-time Interaction within the plasma

14 Modified matrix element 

15 Modified matrix element squared

16 Differential rate

17 Elementary scattering process

18 Auxiliary functions for average over velocity directions

19 Summary  Incorporate an explicit conserved current into the description of collisional energy loss  The above requires considering the time the current spends within the plasma  Predictions?... Not yet, working on them.


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