/master/JETSCAPE/src/jet/

Name	Size	Date (UTC)	Last indexed	Description
Name	Size	Date (UTC)	Last indexed	Description
Parent directory	-	2026-04-02 08:00:30
Martini/	-	2026-04-02 08:00:30		the files logEnDtrqq and logEnDtrqg contain the transition rates dGamma/domega for qq->qq and qg->qg as functions of alpha_s and omega. Temperature scales out (so when using omega/T, this will give you the transition rate at temperature T) Also, in the approximation used (method B in my paper with Charles and Guangyou), the energy dependence (E of the jet) is only in the cutoff (omega<q<E). So no E dependence here - just cut off the data at omega=E when using it. To get the rate for gq->gq and gg->gg just multiply the rates for qq->qq or qg->qg respectively by 9/4. In the used approximation this is exact. alpha_s runs from 0.15 to 0.45 in 0.03 steps. linearly. omega runs from -Exp(6.8) to +Exp(6.8) where the exponent changes in 0.2 steps from -5 to 6.8 both on the positive and on the negative side. omega is given explicitly in the file, and so is alpha_s
AdSCFT.cc	10451 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
AdSCFT.h	1871 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
AdSCFTMutex.cc	624 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07	include <vector>
AdSCFTMutex.h	394 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07	ifndef
ElossValidation.cc	4437 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
ElossValidation.h	1031 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
HadronPrinter.cc	1877 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
HadronPrinter.h	1662 bytes	2026-04-02 08:00:30	2026-04-02 08:15:07
LBT.cc	145814 bytes	2026-04-02 08:00:30	2026-04-02 08:15:09
LBT.h	14630 bytes	2026-04-02 08:00:30	2026-04-02 08:15:09
LBTMutex.cc	618 bytes	2026-04-02 08:00:30	2026-04-02 08:15:09	include <vector>
LBTMutex.h	379 bytes	2026-04-02 08:00:30	2026-04-02 08:15:09	ifndef
Martini.cc	124317 bytes	2026-04-02 08:00:30	2026-04-02 08:15:10
Martini.h	6032 bytes	2026-04-02 08:00:30	2026-04-02 08:15:10
MartiniMutex.cc	626 bytes	2026-04-02 08:00:30	2026-04-02 08:15:10	include <vector>
MartiniMutex.h	399 bytes	2026-04-02 08:00:30	2026-04-02 08:15:10	ifndef
Matter.cc	170292 bytes	2026-04-02 08:00:30	2026-04-02 08:15:11
Matter.h	8069 bytes	2026-04-02 08:00:30	2026-04-02 08:15:11
PartonPrinter.cc	3253 bytes	2026-04-02 08:00:30	2026-04-02 08:15:11
PartonPrinter.h	1705 bytes	2026-04-02 08:00:30	2026-04-02 08:15:11

Name

Size

Date (UTC)

Last indexed

Description

Name

Size

Date (UTC)

Last indexed

Description

Parent directory

2026-04-02 08:00:30

Martini/

2026-04-02 08:00:30

the files logEnDtrqq and logEnDtrqg contain the transition rates dGamma/domega for qq->qq and qg->qg as functions of alpha_s and omega. Temperature scales out (so when using omega/T, this will give you the transition rate at temperature T) Also, in the approximation used (method B in my paper with Charles and Guangyou), the energy dependence (E of the jet) is only in the cutoff (omega<q<E). So no E dependence here - just cut off the data at omega=E when using it.
To get the rate for gq->gq and gg->gg just multiply the rates for qq->qq or qg->qg respectively by 9/4. In the used approximation this is exact.
alpha_s runs from 0.15 to 0.45 in 0.03 steps. linearly.
omega runs from -Exp(6.8) to +Exp(6.8) where the exponent changes in 0.2 steps from -5 to 6.8 both on the positive and on the negative side.
omega is given explicitly in the file, and so is alpha_s