V. Uzhinsky, A Galoyan (JINR, Dubna, Russia), 2015

Slides:



Advertisements
Similar presentations
Pawan Kumar NetrakantiPANIC-2005, Santa Fe1 Pion, proton and anti-proton transverse momentum spectra in p+p and d+Au collisions at  s NN = 200 GeV Outline:
Advertisements

Identified particle transverse momentum distributions in 200 GeV Au+Au collisions at RHIC 刘海东 中国科技大学.
Status and Plans for Geant4 Hadronics Dennis Wright (SLAC) SPENVIS & Geant4 Space Users' Workshop Leuven, Belgium 3-7 October 2005.
Pion yield studies for proton drive beams of 2-8 GeV kinetic energy for stopped muon and low-energy muon decay experiments Sergei Striganov Fermilab Workshop.
James Ritman Univ. Giessen PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter Overview of the PANDA Pbar-A Program The Pbar Facility.
 Transverse Polarization in STAR Au-Au Collisions Polarization definition and models E896 results STAR analysis STAR results Significance of results Future.
Monte Carlo 2005, Chattanooga Parton String Models in Geant4 Gunter Folger, Johannes-Peter Wellisch CERN PH/SFT.
Ion Transport Simulation using Geant4 Hadronic Physics
D. Toivonen, M. Tokarev JINR, Dubna Z-scaling & High- pT and cumulative particle production in pp and pA collisions at high energies Z XXXII International.
Fritiof (FTF) model in Geant4, latest improvements V. Uzhinsky (Geant4 hadronic working group) EUDET Annual meeting, HARP-CDP hadroproduction.
Kinematics of  + n   p   0  p reaction Susumu Oda 2007/04/10-19.
Self-similarity of hadron production in pp and AA collisions at high energies D.A. Artemenkov, G.I. Lykasov, A.I. Malakhov Joint Institute for Nuclear.
1 Pion production in np collisions at 1.25AGeV A.Kurilkin, P.Kurilkin, V.Ladygin, A.Ierusalimov, T.Vasiliev, LHEP-JINR, Dubna, Russia For the HADES collaboration.
Geant4 Hadronic |Physics Models Geant4 Tutorial CERN, May 2005 Gunter Folger.
22 nd Winter Workshop on Nuclear Dynamics “Can STAR p+p data help constrain fragmentation functions for strange hadrons” Mark Heinz (for the STAR collaboration)
Charged Kaon Production Yield Studies with Stretcher Sergei Striganov Fermilab Future of Kaon Physics at Fermilab August 21, Fermilab.
A.Galoyan Strange particles production in Pbar-P and Pbar-A Interactions according to FTF model Content 1.Cross sections of Pbar-P processes.
Marina Golubeva, Alexander Ivashkin Institute for Nuclear Research RAS, Moscow AGeV simulations with Geant4 and Shield Geant4 with Dpmjet-2.5 interface.
INVESTIGATION OF MULTIPLE PRODUCTION OF HADRONS IN ANTIPROTON-PROTON AND PROTON-PROTON INTERACTIONS AT 22.4, 32 AND 69 GeV/c. E.G.Boos, N.S.Pokrovsky,
1 The Fritiof (FTF) Model in Geant4 V. Uzhinsky, B. Andersson et al., Nucl. Phys. B281 (1987) 289; B. Nilsson-Almquist and E. Stenlund, Comp.
Generator of PP-elastic scattering events A. Galoyan 18/3/ Simulations of elastic P-P and Pbar-P interactions in frame of Unified systematics of.
A. Galoyan, V. Uzhinsky 1 Reconstruction of FTF generated events with hyperon-antihyperon production 1. Cross sections of Pbar-P processes in FTF model.
Krešo Kadija Ruđer Bošković Institute, Zagreb,Croatia
A. Galoyan and V. Uzhinsky, 22 Окт,2013
Blast-wave fits with resonances to pt spectra from Pb+Pb collisions at √sNN = 2.76 TeV Ivan Meloa,b, Boris Tomášikb,c aŽilinská Univerzita, Žilina, Slovakia.
Recent Developments in Fritiof (FTF) Model V. Uzhinsky,
Improvement and tuning of DPM model
RADIATIVE CORRECTIONS TO IN PANDAROOT
Mark T. Heinz Yale University
Improvement of DPM Generator
Toward understanding of the MIPP data
Study of Hypernuclei with Heavy Ion Beams (HypHI) at GSI Shizu Minami GSI, Germany on behalf of HypHI collaboration Introduction Phase 0 experiment R.
FTF Model in the Last Release G4 9.6.beta
Application of FTF model for simulation of Pbar-P and
Status of FTF validation
into three pions Opportunities in p pbar annihilation S. Ong IPN Orsay
V. Uzhinsky, 25 July 2017 Content Smearing of resonance masses
Unified systematic of elastic Pbar-P, Pbar-A A.Galoyan and V. Uzhinsky
Bugs fixing in UrQMD 1.3 and 2.3
How to Simulate Anti-Matter – Matter Interactions?
Description of strange particle production in Pbar-P and Pbar-A
Selected Problems of Relativistic Nuclear Physics and Multiple Particle Production
Report to Delta Review: Hadronic Validation
Event generators.
G. Arnison et al., UA1 Collaboration
Soft Physics at Forward Rapidity
String Parton Models in Geant4
VEPP-2000 plans for the study of the nucleon form factors
Geant4 FTF model validation for strange particle production
Tatsuya Chujo for the PHENIX collaboration
In search of K+K- molecule
Bedanga Mohanty,VECC, Kolkata (Pawan Kumar Netrakanti and Zhangbu Xu
Main ingredient of the Fritiof model Fritiof model in Geant4
Yields & elliptic flow of and in Au+Au collisions at
Modification of Fragmentation Function in Strong Interacting Medium
Hadron Suppression and Nuclear kT Enhancement Studied with Neutral Pions from p+C, p+Pb, and Pb+Pb Collisions at sNN = 17.3 GeV Quark Matter 2006.
Introduction Results Methods Conclusions
Large-X PDFs in the Drell-Yan Process
Search for f-N Bound State in Jefferson Lab Hall-B
Tatsuya Chujo University of Tsukuba (for the PHENIX Collaboration)
Ministère de la Recherche,
Analysis of <pT>-Nch Correlations in pp and pp Collisions
Fragmentation or Recombination at High pT?
NKS2 Meeting with Bydzovsky NKS2 Experiment / Analysis Status
Identified Charged Hadron
High-energy deuteron cross-sections.
Experiment (Jlab Exp : CLAS eg3)
Search for the onset of baryon anomaly at RHIC-PHENIX
Identified Charged Hadron Production
Spin Studies via Drell-Yan Process at PANDA
Presentation transcript:

V. Uzhinsky, A Galoyan (JINR, Dubna, Russia), 2015 FTF Model for Simulation of Antiproton-proton and Antiproton-nucleus Interactions V. Uzhinsky, A Galoyan (JINR, Dubna, Russia), 2015 In 2002 Jim Ritman and Serge Gonzhur asked us to create background event generator for PANDA experiment. We created DPM generator based on Dual Parton Model, and after that annihilation module in GEANT4 (G4FTFAnnihilation, FTF). Physics Book of PANDA Collaboration, Physics Performance Report for PANDA (AntiProton Annihilations at Darmstadt) Strong Interaction Studies with Antiprotons Main problems: Estimation of the cross sections and string fragmentation.

PbarP processes, Reggeon approach (A.B. Kaidalov) Calculation procedure: V.V. Uzhinsky and A.S. Galoyan, hep-ph/0212369 (2002) Cross-sections of various processes in anti-P P interactions. Implementation: A.Galoian and V.Uzhinsky, AIP Conf.Proc.796:79,2005 New Monte Carlo implementation of quark- Gluon string model of anti-p p interactions. 2

Cross sections, process “b”, anti-di-quark – di-quark string creation 2-particle decay 4

4 Cross sections, process “e”, anti-quark – quark string creation LUND Model Jetset 6.2 4

Cross sections, process “e”, anti-quark – quark string creation 5

Cross sections, process “a”, 3 anti-quark – quark string creation Main channels of anti-proton-proton interactions are reproduced! 6

Cross sections, process “g/h”, high energy interactions 7

8 Validation of FTF, PbarP annihilation at rest See more data in: C. Amsler F. Myhrer Ann. Rev. Nucl. Part. Sci. v. 41 (1991) 219. C. Amsler Rev. Mod. Phys. 70 (1998) 1293 8

9 Pbar-P channel cross sections with baryons in final states Results for ref: 09-06-ref-03, see more details at: http://g4validation.fnal.gov:8080/G4ValidationWebApp/G4ValHAD.jsp 9

Pbar P annihilation channel cross sections Results for ref: 09-06-ref-03 , see more details at: http://g4validation.fnal.gov:8080/G4ValidationWebApp/G4ValHAD.jsp 10

Rapidity distributions of pi- mesons in Pbar-P interactions. Results for inclusive cross sections of anti-Proton – Proton reactions Rapidity distributions of pi- mesons in Pbar-P interactions. G.D. Patel et al., Z. Phys. C - Particles and Fields 12,189, 1982 C.P. Ward et al., Nucl. Phys. B153 299 1979 E.E. Zabrodin et al., Phys. Rev.D, V52, N3, 1995 11

Results for inclusive cross sections of anti-Proton – Proton reactions Rapidity distributions of pi+ mesons in Pbar-P interactions in a wide energy range 12

Results for inclusive cross sections of anti-Proton–Proton reactions PT2 of Pi+ mesons PT2 of Protons 13

E.V. Vlasov, Z. Phys. C - Particles and Fields 13, 95, 1982 Results for inclusive cross sections of anti-Proton–Proton reactions Rapidity distributions of protons E.V. Vlasov, Z. Phys. C - Particles and Fields 13, 95, 1982 G.D. Patel et al., Z. Phys. C - Particles and Fields 12,189, 1982 J. Chyla, Czech. J. Phys. B 30 1980 E .G. Boos et al., Nucl. Phys. B174 45, 1980 14

Description of p+p -> p + X reactions 15 V. Uzhinsky, arXiv: 1404.202 Effect of uu diquark suppression in proton splitting in Monte Carlo event generators V. Uzhinsky, A. Galoyan Phys.Rev. D91 (2015) 3, 037501 xF distributions of protons in pp interactions at 158 GeV/c. Closed points are the NA49 experimental data [5]. Lines are results of FTF model simulations: standard proton splitting (solid black), optimal diquark fragmentation function (dashed red), string inversion (dotted blue), diquark suppression (1/6 instead of 1/3) including the optimal fragmentation function and the string inversion (solid thick).

Antiproton-Nucleus interactions, cross sections for light nuclei V. Uzhinsky, J. Apostolakis , A. Galoyan et al. Phys. Lett. B705 (2011) 235 Anti-proton-nucleus cross sections implemented in Geant4 16 Production cross sections, results for ref: 09-06-ref-03.

Antiproton-Nucleus interactions, cross sections for heavy nuclei V. Uzhinsky, J. Apostolakis , A. Galoyan et al. Phys. Lett. B705 (2011) 235 Anti-proton-nucleus cross sections implemented in Geant4 17 Production cross sections, results for ref: 09-06-ref-03.

Correction of multiplicity of intra-nuclear collisions Antibaryon-Nucleus interactions, inelastic interactions A. Galoyan, Hyperfine Interactions: v. 215 (2013) 69 “Simulations of light antinucleus-nucleus interactions” Low energy, Std. cascade. Cascade+ Resonances Model of nuclear disintegration In high-energy nucleus nucleus interactions. K. Abdel-Waged, V.V. Uzhinsky Phys.Atom.Nucl.60:828-840,1997. High energy, Std. QGS. Correction of multiplicity of intra-nuclear collisions S.Yu. Shmakov, V.V. Uzhinsky, Zeit. fur Phys. C36:77,1987. Max. cross section method: W.A. Coleman: Nucl. Sci. Eng. 32 (1968) 76 18

Antibaryon-Nucleus interactions, inelastic interactions Correction of multiplicity of intra-nuclear collisions, HARP-CDP exp. data Nmax=1, Plab=3, 5 GeV/c: Nmax=2, Plab=8 GeV/c: Nmax=3, Plab=12 19

Annihilation Pbar-A at rest. Cu U Energy spectra of pi+ mesons produced in Pbar–D/Ne at rest J. Rielberger, Nuclear Physics B (Proc Suppl ) 8 (1989) 288-293 20

P.L.McGaughey et al., Phys. Rev. Lett. V56, N20, 1986 21 Results of FTF validation for anti-Proton–Nucleus reactions inflight Momentum distributions of Pi Momentum distributions of Protons P.L.McGaughey et al., Phys. Rev. Lett. V56, N20, 1986 21

Angle and energy distributions of pions and protons in Results of FTF validation for anti-Proton–Nucleus reactions inflight Angle and energy distributions of pions and protons in Pbar-C /Nbar-C interactions at projectile momentum 750 MeV.c P.L.McGaughey et al., Phys. Rev. Lett. V56, N20, 1986 22

Kinetic energy spectra of neutrons produced in Pbar-Al, Pbar-Cu at Results of FTF validation for anti-Proton–Nucleus reactions inflight Kinetic energy spectra of neutrons produced in Pbar-Al, Pbar-Cu at projectile momenta 1.22 GeV/c T. von Egidy et al., Eur. Phys. J. A 8, 197 (2000) LEAR collab. data 23

Kinetic energy spectra of neutrons produced in Pbar-Ta, Pbar-U at Results of FTF validation for anti-Proton–Nucleus reactions inflight Kinetic energy spectra of neutrons produced in Pbar-Ta, Pbar-U at projectile momenta 1.22 GeV/c T. von Egidy et al., Eur. Phys. J. A 8, 197 (2000) LEAR collab. data 24

25 Leading antiproton spectra in PbarA interactions at high energies pA-interactions at 120 GeV/c,R. Bailey et al., Z. Phys. C29 (1985) 1. 25

Rapidity Ch+, Rapidity Ch- mesons Results for FTF validation for Pbar-Nucleus interactions at p= 200 GeV/c Rapidity Ch+, Rapidity Ch- mesons Multi-particle production on hydrogen, argon and xenon targets in a streamer chamber by 200 GeV/c proton and antiproton beams. De Marzo et al. Phys. Rev. D26 (1982) 1019 26

Summary DPM model has been extended to low energies. A new tuning of model parameters have been done. Good description of Pbar+P interactions has been reached. Anti-proton-nucleus cross sections have been calculated and parameterized. Extension of the model on anti-proton-nucleus reactions has been proposed. Promising results have been obtained. Extended model has been implemented in Geant4 toolkit. 27

FTF, Antibaryon-Baryon Interactions 28

Process cross sections 29