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Alice/v1.26t7 v2.26t7 #2

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40 changes: 40 additions & 0 deletions hijing1.383_ampt.f
Original file line number Diff line number Diff line change
Expand Up @@ -3544,6 +3544,22 @@ SUBROUTINE HIJHRD(JP,JT,JOUT,JFLG,IOPJT0)
C ******** JP or JT can not produce jet anymore
C
IF(JOUT.EQ.0) THEN

clin-2/2018 reset energy when energy < |pz| (due to finite precision
c at very high energies for particles with energy ~= beam energy):
if(abs(PP(JP,3)).gt.PP(JP,4)) then
enenew=sqrt(PP(JP,1)**2+PP(JP,2)**2+PP(JP,3)**2+PP(JP,5)**2)
write(6,*) 'reset1:',
1 PP(JP,1),PP(JP,2),PP(JP,3),PP(JP,4),PP(JP,5),enenew
PP(JP,4)=enenew
endif
if(abs(PT(JT,3)).gt.PT(JT,4)) then
enenew=sqrt(PT(JT,1)**2+PT(JT,2)**2+PT(JT,3)**2+PT(JT,5)**2)
write(6,*) 'reset2:',
1 PT(JT,1),PT(JT,2),PT(JT,3),PT(JT,4),PT(JT,5),enenew
PT(JT,4)=enenew
endif
C
EPP=PP(JP,4)+PP(JP,3)
EPM=PP(JP,4)-PP(JP,3)
ETP=PT(JT,4)+PT(JT,3)
Expand Down Expand Up @@ -4871,6 +4887,30 @@ SUBROUTINE HIJSFT(JP,JT,JOUT,IERROR)
IF(WP.LT.0.0 .OR. WM.LT.0.0) GO TO 1000

IF(JOUT.EQ.0) THEN

clin-2/2018 reset energy when energy < |pz| (due to finite precision
c at very high energies for particles with energy ~= beam energy):
if(abs(PP(JP,3)).gt.PP(JP,4)) then
enenew=sqrt(PP(JP,1)**2+PP(JP,2)**2+PP(JP,3)**2+PP(JP,5)**2)
write(6,*) 'reset3:',
1 PP(JP,1),PP(JP,2),PP(JP,3),PP(JP,4),PP(JP,5),enenew
PP(JP,4)=enenew
endif
if(abs(PT(JT,3)).gt.PT(JT,4)) then
enenew=sqrt(PT(JT,1)**2+PT(JT,2)**2+PT(JT,3)**2+PT(JT,5)**2)
write(6,*) 'reset4:',
1 PT(JT,1),PT(JT,2),PT(JT,3),PT(JT,4),PT(JT,5),enenew
PT(JT,4)=enenew
endif
c update variables:
EPP=PP(JP,4)+PP(JP,3)
EPM=PP(JP,4)-PP(JP,3)
ETP=PT(JT,4)+PT(JT,3)
ETM=PT(JT,4)-PT(JT,3)
WP=EPP+ETP
WM=EPM+ETM
SW=WP*WM
C
IF(EPP.LT.0.0) GO TO 1000
IF(EPM.LT.0.0) GO TO 1000
IF(ETP.LT.0.0) GO TO 1000
Expand Down
28 changes: 14 additions & 14 deletions input.ampt
Original file line number Diff line number Diff line change
@@ -1,15 +1,15 @@
200 ! EFRM (sqrt(S_NN) in GeV if FRAME is CMS)
CMS ! FRAME
CMS ! FRAME
A ! PROJ
A ! TARG
197 ! IAP (projectile A number)
79 ! IZP (projectile Z number)
197 ! IAT (target A number)
79 ! IZT (target Z number)
1 ! NEVNT (total number of events)
1 ! NEVNT (total number of events)
0. ! BMIN (mininum impact parameter in fm)
3. ! BMAX (maximum impact parameter in fm, also see below)
4 ! ISOFT (D=1): select Default AMPT or String Melting(see below)
4 ! ISOFT (D=4): select Default AMPT or String Melting(see below)
150 ! NTMAX: number of timesteps (D=150), see below
0.2 ! DT: timestep in fm (hadron cascade time= DT*NTMAX) (D=0.2)
0.55 ! PARJ(41): parameter a in Lund symmetric splitting function
Expand All @@ -20,7 +20,7 @@ A ! TARG
0 ! quenching flag (D=0,no; 1,yes)
2.0 ! quenching parameter -dE/dx (GeV/fm) in case quenching flag=1
2.0 ! p0 cutoff in HIJING for minijet productions (D=2.0)
2.265d0 ! parton screening mass in fm^(-1) (D=2.265d0), see below
2.265d0 ! parton screening mass in fm^(-1) (D=2.265d0), see below
0 ! IZPC: (D=0 forward-angle parton scatterings; 100,isotropic)
0.33d0 ! alpha in parton cascade (D=0.33d0), see parton screening mass
1d6 ! dpcoal in GeV
Expand All @@ -37,8 +37,8 @@ A ! TARG
1 ! choice of cross section assumptions for deuteron reactions
-7. ! Pt in GeV: generate events with >=1 minijet above this value
1000 ! maxmiss (D=1000): maximum # of tries to repeat a HIJING event
3 ! flag to turn off initial and final state radiation (D=3)
1 ! flag to turn off Kt kick (D=1)
3 ! flag on initial and final state radiation (D=3,both yes; 0,no)
1 ! flag on Kt kick (D=1,yes; 0,no)
0 ! flag to turn on quark pair embedding (D=0,no; 1,yes)
7., 0. ! Initial Px and Py values (GeV) of the embedded quark (u or d)
0., 0. ! Initial x & y values (fm) of the embedded back-to-back q/qbar
Expand All @@ -51,17 +51,17 @@ A ! TARG
BMAX: the upper limit HIPR1(34)+HIPR1(35)=19.87fm (dAu), 25.60fm(AuAu).
ISOFT: 1 Default,
4 String Melting.
PARJ(41) & (42): 2.2 & 0.5/GeV^2 used for heavy ion (Au+Au, Pb+Pb) collisions,
while the HIJING values (0.5 & 0.9/GeV^2) describe well
Nch in pp collisions and are used for d-Au collisions.
PARJ(41) & (42): for string melting AMPT, 0.55 & 0.15/GeV^2 are recommended
for top RHIC energies and 0.30 & 0.15/GeV^2 are recommended for
LHC energies (see arXiv:1403.6321 for details).
NTMAX: number of time-steps for hadron cascade.
Use a large value (e.g. 1000) for LHC studies or HBT studies at RHIC.
Using NTMAX=3 effectively turns off hadronic cascade.
Using NTMAX=2 or 3 effectively turns off hadronic cascade.
parton screening mass (in 1/fm): its square is inversely proportional to
the parton cross section. Use D=2.265d0 for 3mb cross section
when alpha in parton cascade is set to 0.33;
(note: 3.2264d0 for 3mb cross section when alpha is set to 0.47).
Using 1d4 effectively turns off parton cascade.
the parton cross section. Use D=2.265d0 for 3mb cross section
when alpha in parton cascade is set to 0.33;
(note: 3.2264d0 for 3mb cross section when alpha is set to 0.47).
Using 1d4 effectively turns off parton cascade.
ihjsed: if =11, take HIJING random seed at runtime so that
every run may be automatically different (see file 'exec').
iksdcy: flag for K0s weak decays for comparison with data.
Expand Down
6 changes: 3 additions & 3 deletions main.f
Original file line number Diff line number Diff line change
Expand Up @@ -123,9 +123,9 @@ PROGRAM AMPT
c HIPR1(10)=7.
c
if(isoft.eq.1) then
amptvn = '1.26t7 (Default)'
amptvn = '1.26t7b (Default)'
elseif(isoft.eq.4) then
amptvn = '2.26t7 (StringMelting)'
amptvn = '2.26t7b (StringMelting)'
else
amptvn = 'Test-Only'
endif
Expand All @@ -135,7 +135,7 @@ PROGRAM AMPT
&11X,'##################################################'/1X,
&10X,'# AMPT (A Multi-Phase Transport) model #'/1X,
&10X,'# Version ',a25, ' #'/1X,
&10X,'# 10/28/2016 #'/1X,
&10X,'# 02/17/2018 #'/1X,
&10X,'##################################################'/1X,
&10X,' ')
c when ihjsed=11: use environment variable at run time for HIJING nseed:
Expand Down
8 changes: 8 additions & 0 deletions readme
Original file line number Diff line number Diff line change
@@ -1,5 +1,13 @@
AMPT Users' Guide

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
2/2018 test version v1.26t7b/v2.26t7b:
* Fixed a bug that causes fatal HIJHRD or HIJSFT error and leads to
an incorrect impact parameter distribution (at sqrt_s>=5.023 TeV)
by resetting the energy in case energy < |pz| (due to finite precision
at very high energies for particles with energy ~= beam energy).
* Updated some explanations in input.ampt.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
5/2016 test version v1.26t7/v2.26t7:
* (w/ GL Ma) Changed the following line in art1f.f to avoid the bug
Expand Down