Application of FTF model for simulation of Pbar-P and Pbar-A Interactions A.Galoyan 27.05.2015 PndBoxGenerator, PndDpmDirect, PndDpmGenerator, PndEvtGenGenerator, PndFlatParticleGenerator., PndFlukaGenerator, PndGasGenerator, PndGiBuuGenerator. PndHypBupGenerator, PndJRGenerator, PndPythia6Generator, PndUrqmdSmmGenerator, EMFFgenerators Geant4 9.5 realese (http://geant4.cern.ch/support/source_archive.shtml) Interactions of anti-baryons (including anti-hyperons) and light anti-nuclei with matter have been implemented in the Fritiof (FTF) model. This model is valid for incident anti-baryon energies from 0 to 1 TeV, and for incident anti-nucleus momenta from 150 MeV/c/nucleon up to 1 TeV/c/nucleon. Corresponding anti-baryon and anti-nuclear cross section classes have also been added. New processes were added to handle inelastic reactions of anti-deuterons, anti-tritons, anti-3He and anti-alphas. (from the release Note) Content 1. Cross sections of Pbar-P processes in DPM and FTF models 2. Comparison of calculations of Pbar-P channels by FTF model with exp. data 3. Comparison of calculations of Pbar-P inclusive cross sections with exp. data 4. Differential cross sections of Λ-Λbar and Λ-Σbar productions in Pbar-P interactions 5. Consideration of Λ and Ks0 kinematical properties produced in Pbar-P reactions 6. Calculations of kinematical properties of particles produced in Pbar-A interactions 7. Cross sections of Λ and Ks0 production in Pbar-Nucleus interactions. 1

FTF generator in PandaRoot PndFtfGen class in PandaRoot/trunk/pgenerators directory pgenerators/FtfEvtGen directory: binmake_FORTRAN.mk main.cc standard_FORTRAN.mk CMakeLists.txt PbarA.mac Test30HadronProduction.c common.mk Ftfmake Test30Material.c PbarP.mac Test30Physics.c README.txt G4DecKineticTracks.c include Test30VSecondaryGenerator.c Include directory: FTFtest1.icc G4DecKineticTracks.hh Test30Physics.hh FTFtest2.icc Test30VSecondaryGenerator.hh FTFtest3.icc Test30HadronProduction.hh FTFtest4.icc Test30Material.hh To compile FTF it is needed to give command: > make –f Ftfmake FTFGen executable file is produced. FTF allows one to generate Pbar – P or Pbar – A events ai energy range from 100 MeV to 1000 GeV 2

Pbar- P processes in DPM model Calculation procedure: V.V. Uzhinsky and A.S. Galoyan, hep-ph/0212369 Cross-sections of various processes in anti-P P interactions. Physics Book of PANDA Collaboration, Physics Performance Report for PANDA (AntiProton Annihilations at Darmstadt) Strong Interaction Studies with Antiprotons 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. 3

Cross sections of Pbar-P processes in FTF model of Geant4

Pbar-P channel cross sections with baryons in final states test22/PbarPchan E.Bracci et al.,CERN/HERA 73-1(1973) 5

Pbar-P annihilation channel cross sections test22/PbarPchan Exp. Data: E.Bracci et al.,CERN/HERA 73-1(1973) 6

Results for inclusive cross sections of Antiproton – Proton reactions Rapidity distributions of pi- mesons in Pbar-P interactions. test22/PbarPinclusive 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 7

Results for inclusive cross sections of Antiproton – Proton reactions Rapidity distributions of pi+ mesons in Pbar-P interactions in a wide energy range 8

Results for inclusive cross sections of AntiProton–Proton reactions Rapidity distributions of protons test22/PbarPinclusive 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, 1982J. Chyla, Czech. J. Phys. B 30 1980 E .G. Boos et al., Nucl. Phys. B174 45, 1980 9

Differential Cross Sections of PbarP->ΛΛbar / ΛΣbar test22/PbarHyperon P. D. Barnes et al., Phys. Rev. C 54 2831 (1996) P. D. Barnes et al., Phys Lett B 246 273 (1990) P. D. Barnes et al., Phys Lett B 189 249 (1987) 10

Differential Cross Sections of PbarP->ΛΛbar / ΛΣbar test22/PbarHyperon P. D. Barnes et al., Phys. Rev. C 54 2831 (1996) P. D. Barnes et al., Phys Lett B 246 273 (1990) P. D. Barnes et al., Phys Lett B 189 249 (1987) 11

Differential Cross Sections of PbarP->ΛΛbar / ΛΣbar at 6 GeV/c test22/PbarHyperon exp. data: H. Becker et al., Nucl. Phys. B141 48 (1978) 12

Differential Cross Sections of PbarP->ΛΛbar at different momenta test22/PbarHyperon exp. data: B. Jayet et al., Nuov. Cim. A45, 371 (1978) 13

Xf and Pt2 distributions of Ks0 in PbarP->Ks0 +X at Plab=0,76 GeV/c Inclusive Cross Sections of PbarP->Λ+X and PbarP->Ks0+X processes test22/PbarHyperon exp.data: S. Banerjee et al., TIFR-BC-78-8 Xf and Pt2 distributions of Ks0 in PbarP->Ks0 +X at Plab=0,76 GeV/c 14

Kinametical disributios of Λ, Λbar, Ks0 produced in PbarP interactions at P=3.6 GeV/c exp data: S. Banerjee et al., TIFR-BC-78-8 15

Kinametical distributions of Λ and Ks0 produced in PbarP interactions at Plab=12 GeV/c exp data: D. Bertrand et al., Nucl. Phys. B 128 365 (1977) 16

Kinametical distributions of Λ and Ks0 produced in PbarP interactions at Plab=22.4 GeV/c exp data: B.V. Batyunya et al., Z. Phys.C 25 213 (1984) 18

Kinametical distributions of Λ and Ks0 produced in PbarP interactions at Plab=100 GeV/c 19 exp data: D.R. Ward et al., Phys. Lett. 62B 237 (1976)

Correction of multiplicity of intra-nuclear collisions Simulation of Antibaryon–Nucleus interactions in FTF model 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 19

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 The same is true for anti-nucleus – nucleus interactions 20

reactions inflight Results of FTF validation for Antiproton–Nucleus Momentum distributions of π+ Momentum distributions of Protons exp data: P.L.McGaughey et al., Phys. Rev. Lett. V56, N20, 1986 21

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

reactions inflight Results of FTF validation for AntiProton–Nucleus 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 Results of FTF validation for Antiproton–Nucleus Kinetic energy spectra of neutrons produced in Pbar-Ta, Pbar-U A. Galoyan, V. Uzhinsky //Contribution to Proceedings of ISHEPP XXII, Dubna 2015 T. von Egidy et al., Eur. Phys. J. A 8, 197 (2000) LEAR collab. data 24

Results of FTF validation for Antiproton–Nucleus reactions Multiplicity distributions of neutrons produced in Pbar-Nucleus at energy 1.22 GeV in FTF and UrQMD models A.S.Galoyan et al., «Scaling and Asymptotical Properties of Slow Neutron Inclusive Cross Sections ...» JETP Lett 2015 exp.data : B. Lott et al., Phys.Rev.C 63 034616 25

interactions at p= 200 GeV/c Results of 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

Production cross sections of Ks0 and Λ and produced in PbarA interactions Plab = 600 MeV/c H2 He4 Ne20 Sigma_Lam 0.65+-0.14 3.67+-0.56 12.3+-2.8 0.0 0.0794696 0.202973 Sigma_Ks0 3.74+-0.56 3.90+-0.53 5.4+-1.1 3.44954 5.88075 12.3137 Plab= 3000 MeV/c H1 H2 Ta Sigma_Lam 0.35+-0.11 0.81+-0.07 145+-0.6 0.356418 0.59467 6.68568 Sigma_Ks0 1.2+-0.05 2.78+-0.15 43.4+-1.2 1.72809 3.85392 62.9568 Plab=4000 MeV/c H1 Ta Sigma_Lam 0.53+-0.05 193+-12 0.730055 11.553 Sigma_Ks 1.90+-0.07 82+-6 2.00127 68.9514 exp data: F. Balestra et al., Nucl. Phys. A526 415 (1991) K. Miyano et al., preprint KEK (1988) 27

Kinametical properties of Λ and Ks0 produced in PbarXe interactions at Plab=200 GeV/c I. Derado et al., Z. Phys. C Particles and Fields 50, 31 36 (1991) 28

Conclusion 1. Inclusive cross sections of Pbar-P processes are calculated in FTF model new Geant4 version: 10-01-ref.03 Good results are obtained in comparison with corresponding exp. data. 2. Differential cross sections of ΛΛbar and ΛΣbar produced in Pbar-P interactions are calculated in FTF model. Anisotropic decay of strings in process b ( diquark- anti-diquark creation ) is included for agreement with corresponding exp. data 3. Kinematical properties of Λ hyperons and Ks0 mesons produced in PbarP processes are calculated in FTF model without and with anizotropic decay and compared with exp. data at different initial momenta. 4. Kinematical properties of protons, pi-mesons are calculated in FTF model in new Geant4 - version. Good description of corresponding exp. data are obtained. 5. Promising results are obtained in comparison of calculated kinetic energy and multiplicity of neutrons produced in antiproton-Nucleus interact. with exp. data 6. Comparison of Λ hyperon production cross sections in Pbar-Nucleus interactions at low and intermediate energies shows that results of FTF+Bic are essentially lower than exp. data. However, calculated Ks0 meson production cross sections are in reasonable agreement with exp. data. 7. Good results are obtained at comparison of exp data with FTF calculations for Λ hyperons and Ks0 mesons produced in Pbar-P interactions at 100 GeV/c and Pbar-Xe interactions at 200 GeV/c. 29

Pbar-A annihilation 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 22

Results for inclusive cross sections of Antiproton–Proton reactions PT2 of Pi+ mesons PT2 of Protons J. Chyla, Czech. J. Phys. B 30 1980 E .G. Boos et al., Nucl. Phys. B174 45, 1980 E.V. Vlasov, Z. Phys. C - Particles and Fields 13, 95, 1982 14

Kinematical distributions of Λ, Λbar, Ks0 produced in PbarP interactions at P=3.6 GeV/c exp data: S. Banerjee et al., TIFR-BC-78-8 13