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| 1 | +5360 ! EFRM (sqrt(S_NN) in GeV if FRAME is CMS) |
| 2 | +CMS ! FRAME |
| 3 | +A ! PROJ |
| 4 | +A ! TARG |
| 5 | +208 ! IAP (projectile A number) |
| 6 | +82 ! IZP (projectile Z number) |
| 7 | +208 ! IAT (target A number) |
| 8 | +82 ! IZT (target Z number) |
| 9 | +1 ! NEVNT (total number of events) - overwritten by generator_AMPT.C |
| 10 | +0. ! BMIN (mininum impact parameter in fm) |
| 11 | +20. ! BMAX (maximum impact parameter in fm, also see below) |
| 12 | +4 ! ISOFT (D=4): select Default AMPT or String Melting(see below) |
| 13 | +1000 ! NTMAX: number of timesteps (D=150), see below |
| 14 | +0.2 ! DT: timestep in fm (hadron cascade time= DT*NTMAX) (D=0.2) |
| 15 | +0.30 ! PARJ(41): parameter a in Lund symmetric splitting function |
| 16 | +0.15 ! PARJ(42): parameter b in Lund symmetric splitting function |
| 17 | +1 ! (D=1,yes;0,no) flag for popcorn mechanism(netbaryon stopping) |
| 18 | +1.0 ! PARJ(5) to control BMBbar vs BBbar in popcorn (D=1.0) |
| 19 | +1 ! shadowing flag (Default=1,yes; 0,no) |
| 20 | +0 ! quenching flag (D=0,no; 1,yes) |
| 21 | +2.0 ! quenching parameter -dE/dx (GeV/fm) in case quenching flag=1 |
| 22 | +2.0 ! p0 cutoff in HIJING for minijet productions (D=2.0) |
| 23 | +3.2264d0 ! parton screening mass in fm^(-1) (D=2.265d0), see below |
| 24 | +0 ! IZPC: (D=0 forward-angle parton scatterings; 100,isotropic) |
| 25 | +0.33d0 ! alpha in parton cascade (D=0.33d0), see parton screening mass |
| 26 | +1d6 ! dpcoal in GeV |
| 27 | +1d6 ! drcoal in fm |
| 28 | +0 ! ihjsed: take HIJING seed from below (D=0)or at runtime(11) - overwritten by generator_AMPT.C |
| 29 | +13150909 ! random seed for HIJING - overwritten by generator_AMPT.C |
| 30 | +8 ! random seed for parton cascade - overwritten by generator_AMPT.C |
| 31 | +0 ! flag for K0s weak decays (D=0,no; 1,yes) |
| 32 | +1 ! flag for phi decays at end of hadron cascade (D=1,yes; 0,no) |
| 33 | +0 ! flag for pi0 decays at end of hadron cascade (D=0,no; 1,yes) |
| 34 | +0 ! optional OSCAR output (D=0,no; 1,yes; 2&3,more parton info) |
| 35 | +0 ! flag for perturbative deuteron calculation (D=0,no; 1or2,yes) |
| 36 | +1 ! integer factor for perturbative deuterons(>=1 & <=10000) |
| 37 | +1 ! choice of cross section assumptions for deuteron reactions |
| 38 | +-7. ! Pt in GeV: generate events with >=1 minijet above this value |
| 39 | +1000 ! maxmiss (D=1000): maximum # of tries to repeat a HIJING event |
| 40 | +3 ! flag on initial and final state radiation (D=3,both yes; 0,no) |
| 41 | +1 ! flag on Kt kick (D=1,yes; 0,no) |
| 42 | +0 ! flag to turn on quark pair embedding (D=0,no; 1,yes) |
| 43 | +7., 0. ! Initial Px and Py values (GeV) of the embedded quark (u or d) |
| 44 | +0., 0. ! Initial x & y values (fm) of the embedded back-to-back q/qbar |
| 45 | +1, 5., 0. ! nsembd(D=0), psembd (in GeV),tmaxembd (in radian). |
| 46 | +0 ! Flag to enable users to modify shadowing (D=0,no; 1,yes) |
| 47 | +1.d0 ! Factor used to modify nuclear shadowing |
| 48 | +1 ! Flag for random orientation of reaction plane (D=0,no; 1,yes) |
| 49 | + |
| 50 | +%%%%%%%%%% O2DPG notes: |
| 51 | +Pb-Pb at sqrt(s_NN) = 5.36 TeV, minimum bias (b = 0-20 fm), String Melting |
| 52 | +with the LHC settings of arXiv:1403.6321 (a=0.30, b=0.15/GeV^2, 1.5 mb parton |
| 53 | +cross section: alpha=0.33 and screening mass 3.2264/fm). |
| 54 | +Values are read by AMPT line by line: do NOT add or remove lines above. |
| 55 | +NEVNT (line 9), ihjsed (line 28) and the two seeds (lines 29-30) are |
| 56 | +overwritten by MC/config/common/external/generator/generator_AMPT.C. |
| 57 | +%%%%%%%%%% Further explanations: |
| 58 | +BMAX: the upper limit HIPR1(34)+HIPR1(35)=19.87fm (dAu), 25.60fm(AuAu). |
| 59 | +ISOFT: 1 Default, |
| 60 | + 4 String Melting. |
| 61 | +PARJ(41) & (42): for string melting AMPT, 0.55 & 0.15/GeV^2 are recommended |
| 62 | + for top RHIC energies and 0.30 & 0.15/GeV^2 are recommended for |
| 63 | + LHC energies (see arXiv:1403.6321 for details). |
| 64 | +NTMAX: number of time-steps for hadron cascade. |
| 65 | + Use a large value (e.g. 1000) for LHC studies or HBT studies at RHIC. |
| 66 | + Using NTMAX=2 or 3 effectively turns off hadronic cascade. |
| 67 | +parton screening mass (in 1/fm): its square is inversely proportional to |
| 68 | + the parton cross section. Use D=2.265d0 for 3mb cross section |
| 69 | + when alpha in parton cascade is set to 0.33; |
| 70 | + (note: 3.2264d0 for 3mb cross section when alpha is set to 0.47). |
| 71 | + Using 1d4 effectively turns off parton cascade. |
| 72 | +ihjsed: if =11, take HIJING random seed at runtime so that |
| 73 | + every run may be automatically different (see file 'exec'). |
| 74 | +iksdcy: flag for K0s weak decays for comparison with data. |
| 75 | +iphidcy: flag for phi meson decays at the end of hadron cascade for comparison |
| 76 | + with data; default is yes; use 0 to turn off these decays. |
| 77 | + Note: phi meson decay during hadron cascade is always enabled. |
| 78 | +ipi0dcy: flag for pi0 electromagnetic decays at the end of hadron cascade for |
| 79 | + comparison with data; set to 1 to turn on pi0 decays. |
| 80 | +ioscar: 0 Dafault, |
| 81 | + 1 Write output in the OSCAR format, |
| 82 | + 2 Write out the complete parton information |
| 83 | + (ana/parton-initial-afterPropagation.dat) |
| 84 | + right after string melting (before parton cascade), |
| 85 | + 3 Write out several more files on parton information (see readme). |
| 86 | +idpert: flag for perturbative deuteron and antideuteron calculations |
| 87 | + with results in ana/ampt_pert.dat: |
| 88 | + 0 No perturbative calculations, |
| 89 | + 1 Trigger a production of NPERTD perturbative deuterons |
| 90 | + in each NN collision, |
| 91 | + 2 Trigger a production of NPERTD perturbative deuterons only in |
| 92 | + an NN collision where a conventional deuteron is produced. |
| 93 | + Note: conventional deuteron calculations are always performed |
| 94 | + with results in ana/ampt.dat. |
| 95 | +NPERTD: number of perturbative deuterons produced in each triggered collision; |
| 96 | + setting it to 0 turns off perturbative deuteron productions. |
| 97 | +idxsec: choose a cross section model for deuteron inelastic/elastic collisions: |
| 98 | + 1: same |matrix element|**2/s (after averaging over initial spins |
| 99 | + and isospins) for B+B -> deuteron+meson at the same sqrt(s); |
| 100 | + 2: same |matrix element|**2/s for B+B -> deuteron+meson |
| 101 | + at the same sqrt(s)-threshold; |
| 102 | + 3: same |matrix element|**2/s for deuteron+meson -> B+B |
| 103 | + at the same sqrt(s); |
| 104 | + 4: same |matrix element|**2/s for deuteron+meson -> B+B |
| 105 | + at the same sqrt(s)-threshold; |
| 106 | + 1 or 3 also chooses the same cross section for deuteron+meson or baryon |
| 107 | + elastic collision at the same sqrt(s); |
| 108 | + 2 or 4 also chooses the same cross section for deuteron+meson or baryon |
| 109 | + elastic collision at the same sqrt(s)-threshold. |
| 110 | +%%%%%%%%%% For jet studies: |
| 111 | +pttrig: generate events with at least 1 initial minijet parton above this Pt |
| 112 | + value, otherwise repeat HIJING event until reaching maxmiss tries; |
| 113 | + use a negative value to disable this requirement and get normal events. |
| 114 | +maxmiss: maximum number of tries for the repetition of a HIJING event to obtain |
| 115 | + a minijet above the Pt value of pttrig; increase maxmiss if some events |
| 116 | + fail to generate at least 1 initial minijet parton above pttrig. |
| 117 | + it is safer to set a large value for high pttrig and/or large b value |
| 118 | + and/or smaller colliding nuclei. |
| 119 | +IHPR2(2): flag to turn off initial and final state radiation: |
| 120 | + 0 both radiation off, 1 only final off, 2 only initial off, 3 both on. |
| 121 | +IHPR2(5): flag to turn off Pt kick due to soft interactions: 0 off, 1 on. |
| 122 | + Setting both IHPR2(2) and IHPR2(5) to zero makes it more likely to |
| 123 | + have two high-Pt minijet partons that are close to back-to-back. |
| 124 | +%%%%%%%%%% To embed a back-to-back light q/qbar jet pair |
| 125 | +%%%%%%%%%% and a given number of soft pions along each jet into each event: |
| 126 | +iembed: flag to turn on quark pair embedding: |
| 127 | + 1: on with fixed position(xembd,pembd) and Pt(pxqembd,pyqembd); |
| 128 | + 2: on with fixed position(xembd,pembd) and random azimuthal angle |
| 129 | + with Pt-magnitude given by sqrt(pxqembd^2+pyqembd^2); |
| 130 | + 3: on with random position and fixed Pt(pxqembd,pyqembd); |
| 131 | + 4: on with random position and random random azimuthal angle |
| 132 | + with Pt-magnitude given by sqrt(pxqembd^2+pyqembd^2); |
| 133 | + for iembed=3 or 4: need a position file "embed-jet-xy.txt"; |
| 134 | + Other integers: off. |
| 135 | +pxqembd, pyqembd: sqrt(pxqembd^2+pyqembd^2) > 70MeV/c is required; |
| 136 | + the embedded quark and antiquark have pz=0. |
| 137 | +xembd, yembd: the embedded quark and antiquark jets have z=0 initially. Note: |
| 138 | + the x-axis is defined as the direction along the impact parameter. |
| 139 | +nsembd: number of soft pions to be embedded with each high-Pt parton |
| 140 | + in the embedded jet pair. |
| 141 | +psembd: Momentum of each embedded soft pion in GeV. |
| 142 | +tmaxembd: maximum angle(rad) of embedded soft pions relative to high-Pt parton. |
| 143 | +%%%%%%%%%% User modification of nuclear shadowing: |
| 144 | +ishadow: set to 1 to enable users to adjust nuclear shadowing |
| 145 | + provided the shadowing flag IHPR2(6) is turned on; default value is 0. |
| 146 | +dshadow: valid when ishadow=1; this parameter modifies the HIJING shadowing |
| 147 | + parameterization Ra(x,r)==1+fa(x,r) via Ra(x,r)==1+fa(x,r)*dshadow, |
| 148 | + so the value of 0.d0 turns off shadowing |
| 149 | + and the value of 1.d0 uses the default HIJING shadowing; |
| 150 | + currently limited to 0.d0<=dshadow<=1.d0 to make sure Ra(x,r)>0. |
| 151 | +iphirp: set to 1 to turn on random orientation of reaction plane (D=0) |
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