Download presentation
Presentation is loading. Please wait.
Published byMeredith Cameron Modified over 6 years ago
1
Unified systematic of elastic Pbar-P, Pbar-A A.Galoyan and V. Uzhinsky
scattering data A.Galoyan and V. Uzhinsky 13/12/2011 ● Application of Glauber theory for antiproton-nucleus interactions ● Our parametrization of Pbar-P total and elastic cross sections ● Glauber amplitudes and black disk model with diffuse boundary approximation ● Effective parameters of the black disk model with diffuse boundary ● Geant4 class “G4AntiNuclElastic” - for simulation of Anti-proton – Nucleus Elastic scattering ● Simulation method of Coulomb and Hadron scatterings ● New parameterization of Anti-P P Elastic Scattering, Imaginary and Real parts of Elastic Scattering Amplitude ● Description of recent Totem data on elastic pp-interactions at 7 TeV ! 1
2
Glauber theory for antiproton-nucleus interactions
adTa_Fig8 Amplitude of hadron-nucleus elastic scattering Differential elastic scattering cross section Amplitude of elastic hN scattering in impact parameter representation ß is the slope parameter of hN differential elastic cross section Square module of the wave function is written as: Diagen: Generator Of Inelastic Nucleus-nucleus Interaction Diagrams. S. Shmakov, V.Uzhinsky, A.Zadorozhny, Comp. Phys. Comm., 54 (1989) 125 2
3
Our parameterization of PbarP cross sections
σel/σtot=1/(2 Csh)≈1/3, according to the quasi-eikonal approach of the reggeon field theory (K.A. Ter-Martirosyan, A.B. Kaidalov) 3
4
V. Uzhinsky, J. Apostolakis, A. Galoyan et al. , Phys
V. Uzhinsky, J. Apostolakis, A. Galoyan et al., Phys. Lett B705 (2011) 235 Calculation results in G4ComponentAntiNuclNuclearXS, Pbar – Nuclei 4
5
Calculation results for Profile functions in Glauber model
Generator of inelastic nucleus-nucleus interaction diagrams Computer Physics Communications, 54 (1989)125 S. Yu. Shmakov, V. V. Uzhinskii, A. M. Zadorozhny Profile functions P(b) for pbar+Pb at Plab=0.1, 1, 1000 GeV/c According to black disk model approximation 2-dimensional Fourie transform of P(b): (1) W.E. Frahn, R.H. Venter// Ann. Phys. 24 (1963) 234; D.C. Choudhury// Phys. Rev. C22 (1980) 1848; 5 Yu.A. Berezhnoy, V.Yu. Korda// Inter. J. Mod. Phys. 7 (1998) 723
6
Glauber amplitudes and black disk model approximation
Pbar+Pb elastic scattering Glauber amplitudes at P=0.1 and 1000GeV/c (blue lines) and J1(Rq)/(Rq) (black lines) First zero of F(q) can be used for determination of R, R=3.832/q_zero F(0)=πR2 at such choice of R 6
7
Interpolation of effective parameters of black disk model
7
8
Interpolation of Effective parameters of black disk model
8
9
Class: G4VHadronElastic G4AntiNuclElastic Data of class: Base class
GEANT4 Class: G4VHadronElastic Base class Class for elastic Pbar-P, Pbar-A simulations G4AntiNuclElastic G4double SampleInvariantT ( const G4ParticleDefinition* p, G4double plab, G4int Z, G4int A); Derived methods Sampling of polar angle Theta Methods: G4double SampleThetaCMS( particle, plab, Z, A); G4double SampleThetaLab( p, plab, Z, A); and other methods cs, fTeta1, fTetaCMS, fThetaLab, fRa, fRef et al. Data of class: 9
10
SampleInvariantT (p, plab, Z, A);
G4AntiNuclElastic:: SampleInvariantT (p, plab, Z, A); Coulomb – Wentzel scattering ( V.M. Grishine/ CPC 181 (2010) 921 ) Hadronic part ─ Magorant function 10
11
Differential Cross sections of Elastic Pbar Nucleus interactions
11
12
Differential Cross sections of Elastic Pbar Nucleus interactions
12
13
Differential Cross sections of Elastic Pbar Nucleus interactions
13
14
A, Galoyan, J. Ritman, A. Sokolov, V. Uzhinsky// arXiv:0809
A, Galoyan, J. Ritman, A. Sokolov, V. Uzhinsky// arXiv: [hep-ex] Parameterization of the anti-P P Elastic Scattering Differential Cross Section Between 2-GeV/c <= P(lab) <= 16-GeV/c. 14
15
Parameterization of the anti-P P Elastic Scattering Differential Cross Section Between 2-GeV/c <= P(lab) <= 20-GeV/c. 15
16
Real part of elastic pbar-p amplitude. Derivative dispersion relations
New parameterization of anti-P P elastic scattering differential cross section adTa_Fig8 Black disk model approximation with diffuse boundary with Imaginary and Real parts of elastic scattering amplitude Real part of elastic pbar-p amplitude. Derivative dispersion relations J.B. Bronzan, G.L. Kane, U.P. Sukhatme, Phys. Lett. 49B (1974) 227; M.M. Block, R.N. Cahn, Rev. Mod. Phys. 57 (1985) 563 16
17
Fitting results Fitting expression:
adTa_Fig8 94 sets of exp data were used from Plab=181 MeV/c up to sqrt(S)=1800 GeV Fitting results (low energy) Fitting results 17
18
Fitting results (intermediate and high projectile momenta)
94 sets of exp data were used from Plab=181 MeV/c up to sqrt(S)=1800 GeV 18
19
Interpolation of parameters R_eff and c_eff
New parameters of R, C and ρ are implemented Geant4 class: G4AntiNuclElastic 19
20
Interpolation of Ratio of Real to Imaginary parts of the elastic Pbar-P scattering amplitude
“Structure of antiproton-proton elastic scattering amplitude” A. Galoyan, V. Uzhinsky, JETP Letters, v. 94, No 7 (2011) 20
21
Extrapolation results for elastic Pbar-P differential cross sections
21
22
The Totem results, pp-interactions at 7 TeV!
EPL, 95 (2011) 41001, EPL 96 (2011) 21002 Reff=1.07 fm, Ceff=0.375 fm 22
23
Description of the High Momentum Part of the exp. data
V. Uzhinsky, A. Galoyan, Nov e-Print: arXiv: "Description of the Totem experimental data on elastic pp-scattering at sqrt(s)=7 TeV in the framework of unified systematic of elastic scattering data.“ Description of the High Momentum Part of the exp. data At |t|> 2 (GeV/c)2 all the cross sections have the same shape at sqrt(S)> 10 GeV. To reproduce the shape we add to imaginary part of elastic amplitude “hard” part 23
24
Description of the Totem data and our predictions for other LHC En.
V. Uzhinsky, A. Galoyan, Nov e-Print: arXiv: "Description of the Totem experimental data on elastic pp-scattering at sqrt(s)=7 TeV in the framework of unified systematic of elastic scattering data.“ Description of the Totem data and our predictions for other LHC En. 24
25
Conclusion and plans 1. G4 Class G4AntiNuclElastic for simulation of anti-nucleon and anti- nucleus nucleus elastic scattering has been created. The class is based on Black Disk Model with Diffuse Boundary and Coulomb- Wentzel model. Effective parameters “R” and “c” of Black Disk model are found. 3. Differential cross sections of elastic scattering of antiprotons with nuclei were calculated using the class G4AntiNuclElastic. Good description of known exp. data were obtained. New parametrization of antiproton-proton elastic scattering based on the Black Disk Model with Diffuse Boundary taking into account the real part of elastic amplitude is proposed. 5. Exp. data on antiproton-proton elastic scattering are described well. Good results are obtained for recent Totem data! Take into account the real part of PbarP amplitude in simulation of anti-P nucleus elastic scattering. 2. More accurate treating of the Coulomb scattering in the PbarP and Pbar nucleus elastic scatterings . Implementation of new parametrization of antiproton-proton elastic scattering in DPM generator in Panda-Root 25
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.