Theory and phenomenology of the heavy-ion collisions

Department of Physics

Theoretical uncertainties in exclusive electroproduction of S-wave charmonia

This web page provides

If you want to use these datasets, please cite the following:

Contact person: Michal Krelina, michal.krelina@fjfi.cvut.cz

Interpolation c++ interface:
For using the grids, use the following interpolation code: interpol.h and interpol.cpp. Example of using this interpolation method is in test.cpp. All together is possible download in zip file code.zip.

(A) Datasets for vector meson wave functions generated by various realistic q-qbar potentials

VM Name Mass [GeV] n2s+1lJ Pot. Wave function ψ(r) (non-boosted) Wave function ψ(pT,z) (boosted) Wave function ψ(rT,z) (boosted)
J/ψ(1S)3.096913S1HAR
COR
BT
LOG
POW
VM_psi1S_r_HO.grid
VM_psi1S_r_Cor.grid
VM_psi1S_r_BT.grid
VM_psi1S_r_Log.grid
VM_psi1S_r_Pow.grid
VM_psi1S_kz_HO.grid
VM_psi1S_kz_Cor.grid
VM_psi1S_kz_BT.grid
VM_psi1S_kz_Log.grid
VM_psi1S_kz_Pow.grid
VM_psi1S_rz_HO.grid
VM_psi1S_rz_Cor.grid
VM_psi1S_rz_BT.grid
VM_psi1S_rz_Log.grid
VM_psi1S_rz_Pow.grid
ψ(2S)3.68609723S1HAR
COR
BT
LOG
POW
VM_psi2S_r_HO.grid
VM_psi2S_r_Cor.grid
VM_psi2S_r_BT.grid
VM_psi2S_r_Log.grid
VM_psi2S_r_Pow.grid
VM_psi2S_kz_HO.grid
VM_psi2S_kz_Cor.grid
VM_psi2S_kz_BT.grid
VM_psi2S_kz_Log.grid
VM_psi2S_kz_Pow.grid
VM_psi2S_rz_HO.grid
VM_psi2S_rz_Cor.grid
VM_psi2S_rz_BT.grid
VM_psi2S_rz_Log.grid
VM_psi2S_rz_Pow.grid
Υ(1S)9.4613S1HAR
COR
BT
LOG
POW
VM_upsilon1S_r_HO.grid
VM_upsilon1S_r_Cor.grid
VM_upsilon1S_r_BT.grid
VM_upsilon1S_r_Log.grid
VM_upsilon1S_r_Pow.grid
VM_upsilon1S_kz_HO.grid
VM_upsilon1S_kz_Cor.grid
VM_upsilon1S_kz_BT.grid
VM_upsilon1S_kz_Log.grid
VM_upsilon1S_kz_Pow.grid
VM_upsilon1S_rz_HO.grid
VM_upsilon1S_rz_Cor.grid
VM_upsilon1S_rz_BT.grid
VM_upsilon1S_rz_Log.grid
VM_upsilon1S_rz_Pow.grid
Υ(2S)10.0232623S1HAR
COR
BT
LOG
POW
VM_upsilon2S_r_HO.grid
VM_upsilon2S_r_Cor.grid
VM_upsilon2S_r_BT.grid
VM_upsilon2S_r_Log.grid
VM_upsilon2S_r_Pow.grid
VM_upsilon2S_kz_HO.grid
VM_upsilon2S_kz_Cor.grid
VM_upsilon2S_kz_BT.grid
VM_upsilon2S_kz_Log.grid
VM_upsilon2S_kz_Pow.grid
VM_upsilon2S_rz_HO.grid
VM_upsilon2S_rz_Cor.grid
VM_upsilon2S_rz_BT.grid
VM_upsilon2S_rz_Log.grid
VM_upsilon2S_rz_Pow.grid
Υ(3S)10.355233S1HAR
COR
BT
LOG
POW
VM_upsilon3S_r_HO.grid
VM_upsilon3S_r_Cor.grid
VM_upsilon3S_r_BT.grid
VM_upsilon3S_r_Log.grid
VM_upsilon3S_r_Pow.grid
VM_upsilon3S_kz_HO.grid
VM_upsilon3S_kz_Cor.grid
VM_upsilon3S_kz_BT.grid
VM_upsilon3S_kz_Log.grid
VM_upsilon3S_kz_Pow.grid
VM_upsilon3S_rz_HO.grid
VM_upsilon3S_rz_Cor.grid
VM_upsilon3S_rz_BT.grid
VM_upsilon3S_rz_Log.grid
VM_upsilon3S_rz_Pow.grid

(B) Datasets for integrated electroproduction cross sections with/without spin rotation (SR)

VM Name Pot SR γp → VMp tot x-sec (GBW) γp → VMp tot x-sec (GBWnew) γp → VMp tot x-sec (IP-Sat) γp → VMp tot x-sec (BGBK) γp → VMp tot x-sec (KST)
  J/ψ(1S)  HAR

COR

BT

LOG

POW

Yes
No
Yes
No
Yes
No
Yes
No
Yes
No
tot_psi1S_SR_GBW_HO.grid
tot_psi1S_noSR_GBW_HO.grid
tot_psi1S_SR_GBW_Cor.grid
tot_psi1S_noSR_GBW_Cor.grid
tot_psi1S_SR_GBW_BT.grid
tot_psi1S_noSR_GBW_BT.grid
tot_psi1S_SR_GBW_Log.grid
tot_psi1S_noSR_GBW_Log.grid
tot_psi1S_SR_GBW_Pow.grid
tot_psi1S_noSR_GBW_Pow.grid
tot_psi1S_SR_GBWnew_HO.grid
tot_psi1S_noSR_GBWnew_HO.grid
tot_psi1S_SR_GBWnew_Cor.grid
tot_psi1S_noSR_GBWnew_Cor.grid
tot_psi1S_SR_GBWnew_BT.grid
tot_psi1S_noSR_GBWnew_BT.grid
tot_psi1S_SR_GBWnew_Log.grid
tot_psi1S_noSR_GBWnew_Log.grid
tot_psi1S_SR_GBWnew_Pow.grid
tot_psi1S_noSR_GBWnew_Pow.grid
tot_psi1S_SR_IPSat_HO.grid
tot_psi1S_noSR_IPSat_HO.grid
tot_psi1S_SR_IPSat_Cor.grid
tot_psi1S_noSR_IPSat_Cor.grid
tot_psi1S_SR_IPSat_BT.grid
tot_psi1S_noSR_IPSat_BT.grid
tot_psi1S_SR_IPSat_Log.grid
tot_psi1S_noSR_IPSat_Log.grid
tot_psi1S_SR_IPSat_Pow.grid
tot_psi1S_noSR_IPSat_Pow.grid
tot_psi1S_SR_BGBK_HO.grid
tot_psi1S_noSR_BGBK_HO.grid
tot_psi1S_SR_BGBK_Cor.grid
tot_psi1S_noSR_BGBK_Cor.grid
tot_psi1S_SR_BGBK_BT.grid
tot_psi1S_noSR_BGBK_BT.grid
tot_psi1S_SR_BGBK_Log.grid
tot_psi1S_noSR_BGBK_Log.grid
tot_psi1S_SR_BGBK_Pow.grid
tot_psi1S_noSR_BGBK_Pow.grid
tot_psi1S_SR_KST_HO.grid
tot_psi1S_noSR_KST_HO.grid
tot_psi1S_SR_KST_Cor.grid
tot_psi1S_noSR_KST_Cor.grid
tot_psi1S_SR_KST_BT.grid
tot_psi1S_noSR_KST_BT.grid
tot_psi1S_SR_KST_Log.grid
tot_psi1S_noSR_KST_Log.grid
tot_psi1S_SR_KST_Pow.grid
tot_psi1S_noSR_KST_Pow.grid
  ψ(2S)  HAR

COR

BT

LOG

POW

Yes
No
Yes
No
Yes
No
Yes
No
Yes
No
tot_psi2S_SR_GBW_HO.grid
tot_psi2S_noSR_GBW_HO.grid
tot_psi2S_SR_GBW_Cor.grid
tot_psi2S_noSR_GBW_Cor.grid
tot_psi2S_SR_GBW_BT.grid
tot_psi2S_noSR_GBW_BT.grid
tot_psi2S_SR_GBW_Log.grid
tot_psi2S_noSR_GBW_Log.grid
tot_psi2S_SR_GBW_Pow.grid
tot_psi2S_noSR_GBW_Pow.grid
tot_psi2S_SR_GBWnew_HO.grid
tot_psi2S_noSR_GBWnew_HO.grid
tot_psi2S_SR_GBWnew_Cor.grid
tot_psi2S_noSR_GBWnew_Cor.grid
tot_psi2S_SR_GBWnew_BT.grid
tot_psi2S_noSR_GBWnew_BT.grid
tot_psi2S_SR_GBWnew_Log.grid
tot_psi2S_noSR_GBWnew_Log.grid
tot_psi2S_SR_GBWnew_Pow.grid
tot_psi2S_noSR_GBWnew_Pow.grid
tot_psi2S_SR_IPSat_HO.grid
tot_psi2S_noSR_IPSat_HO.grid
tot_psi2S_SR_IPSat_Cor.grid
tot_psi2S_noSR_IPSat_Cor.grid
tot_psi2S_SR_IPSat_BT.grid
tot_psi2S_noSR_IPSat_BT.grid
tot_psi2S_SR_IPSat_Log.grid
tot_psi2S_noSR_IPSat_Log.grid
tot_psi2S_SR_IPSat_Pow.grid
tot_psi2S_noSR_IPSat_Pow.grid
tot_psi2S_SR_BGBK_HO.grid
tot_psi2S_noSR_BGBK_HO.grid
tot_psi2S_SR_BGBK_Cor.grid
tot_psi2S_noSR_BGBK_Cor.grid
tot_psi2S_SR_BGBK_BT.grid
tot_psi2S_noSR_BGBK_BT.grid
tot_psi2S_SR_BGBK_Log.grid
tot_psi2S_noSR_BGBK_Log.grid
tot_psi2S_SR_BGBK_Pow.grid
tot_psi2S_noSR_BGBK_Pow.grid
tot_psi2S_SR_KST_HO.grid
tot_psi2S_noSR_KST_HO.grid
tot_psi2S_SR_KST_Cor.grid
tot_psi2S_noSR_KST_Cor.grid
tot_psi2S_SR_KST_BT.grid
tot_psi2S_noSR_KST_BT.grid
tot_psi2S_SR_KST_Log.grid
tot_psi2S_noSR_KST_Log.grid
tot_psi2S_SR_KST_Pow.grid
tot_psi2S_noSR_KST_Pow.grid
  Υ(1S)  HAR

COR

BT

LOG

POW

Yes
No
Yes
No
Yes
No
Yes
No
Yes
No
tot_upsilon1S_SR_GBW_HO.grid
tot_upsilon1S_noSR_GBW_HO.grid
tot_upsilon1S_SR_GBW_Cor.grid
tot_upsilon1S_noSR_GBW_Cor.grid
tot_upsilon1S_SR_GBW_BT.grid
tot_upsilon1S_noSR_GBW_BT.grid
tot_upsilon1S_SR_GBW_Log.grid
tot_upsilon1S_noSR_GBW_Log.grid
tot_upsilon1S_SR_GBW_Pow.grid
tot_upsilon1S_noSR_GBW_Pow.grid
tot_upsilon1S_SR_GBWnew_HO.grid
tot_upsilon1S_noSR_GBWnew_HO.grid
tot_upsilon1S_SR_GBWnew_Cor.grid
tot_upsilon1S_noSR_GBWnew_Cor.grid
tot_upsilon1S_SR_GBWnew_BT.grid
tot_upsilon1S_noSR_GBWnew_BT.grid
tot_upsilon1S_SR_GBWnew_Log.grid
tot_upsilon1S_noSR_GBWnew_Log.grid
tot_upsilon1S_SR_GBWnew_Pow.grid
tot_upsilon1S_noSR_GBWnew_Pow.grid
tot_upsilon1S_SR_IPSat_HO.grid
tot_upsilon1S_noSR_IPSat_HO.grid
tot_upsilon1S_SR_IPSat_Cor.grid
tot_upsilon1S_noSR_IPSat_Cor.grid
tot_upsilon1S_SR_IPSat_BT.grid
tot_upsilon1S_noSR_IPSat_BT.grid
tot_upsilon1S_SR_IPSat_Log.grid
tot_upsilon1S_noSR_IPSat_Log.grid
tot_upsilon1S_SR_IPSat_Pow.grid
tot_upsilon1S_noSR_IPSat_Pow.grid
tot_upsilon1S_SR_BGBK_HO.grid
tot_upsilon1S_noSR_BGBK_HO.grid
tot_upsilon1S_SR_BGBK_Cor.grid
tot_upsilon1S_noSR_BGBK_Cor.grid
tot_upsilon1S_SR_BGBK_BT.grid
tot_upsilon1S_noSR_BGBK_BT.grid
tot_upsilon1S_SR_BGBK_Log.grid
tot_upsilon1S_noSR_BGBK_Log.grid
tot_upsilon1S_SR_BGBK_Pow.grid
tot_upsilon1S_noSR_BGBK_Pow.grid
tot_upsilon1S_SR_KST_HO.grid
tot_upsilon1S_noSR_KST_HO.grid
tot_upsilon1S_SR_KST_Cor.grid
tot_upsilon1S_noSR_KST_Cor.grid
tot_upsilon1S_SR_KST_BT.grid
tot_upsilon1S_noSR_KST_BT.grid
tot_upsilon1S_SR_KST_Log.grid
tot_upsilon1S_noSR_KST_Log.grid
tot_upsilon1S_SR_KST_Pow.grid
tot_upsilon1S_noSR_KST_Pow.grid
  Υ(2S)  HAR

COR

BT

LOG

POW

Yes
No
Yes
No
Yes
No
Yes
No
Yes
No
tot_upsilon2S_SR_GBW_HO.grid
tot_upsilon2S_noSR_GBW_HO.grid
tot_upsilon2S_SR_GBW_Cor.grid
tot_upsilon2S_noSR_GBW_Cor.grid
tot_upsilon2S_SR_GBW_BT.grid
tot_upsilon2S_noSR_GBW_BT.grid
tot_upsilon2S_SR_GBW_Log.grid
tot_upsilon2S_noSR_GBW_Log.grid
tot_upsilon2S_SR_GBW_Pow.grid
tot_upsilon2S_noSR_GBW_Pow.grid
tot_upsilon2S_SR_GBWnew_HO.grid
tot_upsilon2S_noSR_GBWnew_HO.grid
tot_upsilon2S_SR_GBWnew_Cor.grid
tot_upsilon2S_noSR_GBWnew_Cor.grid
tot_upsilon2S_SR_GBWnew_BT.grid
tot_upsilon2S_noSR_GBWnew_BT.grid
tot_upsilon2S_SR_GBWnew_Log.grid
tot_upsilon2S_noSR_GBWnew_Log.grid
tot_upsilon2S_SR_GBWnew_Pow.grid
tot_upsilon2S_noSR_GBWnew_Pow.grid
tot_upsilon2S_SR_IPSat_HO.grid
tot_upsilon2S_noSR_IPSat_HO.grid
tot_upsilon2S_SR_IPSat_Cor.grid
tot_upsilon2S_noSR_IPSat_Cor.grid
tot_upsilon2S_SR_IPSat_BT.grid
tot_upsilon2S_noSR_IPSat_BT.grid
tot_upsilon2S_SR_IPSat_Log.grid
tot_upsilon2S_noSR_IPSat_Log.grid
tot_upsilon2S_SR_IPSat_Pow.grid
tot_upsilon2S_noSR_IPSat_Pow.grid
tot_upsilon2S_SR_BGBK_HO.grid
tot_upsilon2S_noSR_BGBK_HO.grid
tot_upsilon2S_SR_BGBK_Cor.grid
tot_upsilon2S_noSR_BGBK_Cor.grid
tot_upsilon2S_SR_BGBK_BT.grid
tot_upsilon2S_noSR_BGBK_BT.grid
tot_upsilon2S_SR_BGBK_Log.grid
tot_upsilon2S_noSR_BGBK_Log.grid
tot_upsilon2S_SR_BGBK_Pow.grid
tot_upsilon2S_noSR_BGBK_Pow.grid
tot_upsilon2S_SR_KST_HO.grid
tot_upsilon2S_noSR_KST_HO.grid
tot_upsilon2S_SR_KST_Cor.grid
tot_upsilon2S_noSR_KST_Cor.grid
tot_upsilon2S_SR_KST_BT.grid
tot_upsilon2S_noSR_KST_BT.grid
tot_upsilon2S_SR_KST_Log.grid
tot_upsilon2S_noSR_KST_Log.grid
tot_upsilon2S_SR_KST_Pow.grid
tot_upsilon2S_noSR_KST_Pow.grid
  Υ(3S)  HAR

COR

BT

LOG

POW

Yes
No
Yes
No
Yes
No
Yes
No
Yes
No
tot_upsilon3S_SR_GBW_HO.grid
tot_upsilon3S_noSR_GBW_HO.grid
tot_upsilon3S_SR_GBW_Cor.grid
tot_upsilon3S_noSR_GBW_Cor.grid
tot_upsilon3S_SR_GBW_BT.grid
tot_upsilon3S_noSR_GBW_BT.grid
tot_upsilon3S_SR_GBW_Log.grid
tot_upsilon3S_noSR_GBW_Log.grid
tot_upsilon3S_SR_GBW_Pow.grid
tot_upsilon3S_noSR_GBW_Pow.grid
tot_upsilon3S_SR_GBWnew_HO.grid
tot_upsilon3S_noSR_GBWnew_HO.grid
tot_upsilon3S_SR_GBWnew_Cor.grid
tot_upsilon3S_noSR_GBWnew_Cor.grid
tot_upsilon3S_SR_GBWnew_BT.grid
tot_upsilon3S_noSR_GBWnew_BT.grid
tot_upsilon3S_SR_GBWnew_Log.grid
tot_upsilon3S_noSR_GBWnew_Log.grid
tot_upsilon3S_SR_GBWnew_Pow.grid
tot_upsilon3S_noSR_GBWnew_Pow.grid
tot_upsilon3S_SR_IPSat_HO.grid
tot_upsilon3S_noSR_IPSat_HO.grid
tot_upsilon3S_SR_IPSat_Cor.grid
tot_upsilon3S_noSR_IPSat_Cor.grid
tot_upsilon3S_SR_IPSat_BT.grid
tot_upsilon3S_noSR_IPSat_BT.grid
tot_upsilon3S_SR_IPSat_Log.grid
tot_upsilon3S_noSR_IPSat_Log.grid
tot_upsilon3S_SR_IPSat_Pow.grid
tot_upsilon3S_noSR_IPSat_Pow.grid
tot_upsilon3S_SR_BGBK_HO.grid
tot_upsilon3S_noSR_BGBK_HO.grid
tot_upsilon3S_SR_BGBK_Cor.grid
tot_upsilon3S_noSR_BGBK_Cor.grid
tot_upsilon3S_SR_BGBK_BT.grid
tot_upsilon3S_noSR_BGBK_BT.grid
tot_upsilon3S_SR_BGBK_Log.grid
tot_upsilon3S_noSR_BGBK_Log.grid
tot_upsilon3S_SR_BGBK_Pow.grid
tot_upsilon3S_noSR_BGBK_Pow.grid
tot_upsilon3S_SR_KST_HO.grid
tot_upsilon3S_noSR_KST_HO.grid
tot_upsilon3S_SR_KST_Cor.grid
tot_upsilon3S_noSR_KST_Cor.grid
tot_upsilon3S_SR_KST_BT.grid
tot_upsilon3S_noSR_KST_BT.grid
tot_upsilon3S_SR_KST_Log.grid
tot_upsilon3S_noSR_KST_Log.grid
tot_upsilon3S_SR_KST_Pow.grid
tot_upsilon3S_noSR_KST_Pow.grid

(A) Generator for vector meson wave functions generated by various realistic q-qbar potentials

Graph type:
Potentials: Harmonic oscillator (HAR)
Cornell potential (COR)
Buchmuller and Tye (BT)
Logarithmic potential (LOG)
Power-law (POW)
Vector meson:
Only for ψ(pT,z) and ψ(rT,z) wave functions:
z LC fraction value: (only 0 < z < 1 values are accepted)


 

(B) Generator for integrated electroproduction cross sections with/without spin rotation

Graph type:
Potentials: Harmonic oscillator (HAR)
Cornell potential (COR)
Buchmuller and Tye (BT)
Logarithmic potential (LOG)
Power-law (POW)
Vector meson:
Dipole cross section: GBW
GBWnew
IPSat
BGBK
KST
x axis type: Q2[GeV2], W [GeV]
W value: [GeV]
Example: if you choose Q2 as an x-axis, you have to fix value of W and vice versa.
B slope value: [GeV-2]
x axis: Min: [GeV2] ; Max: [GeV2] ; lin or log
y axis: Min: [nb]; Max: [nb]; lin or log