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2024年10月30日

PROTON-NUCLEUS SCATTERING IN A THERMODYNAMICAL FIREBALL MODEL

  • We attempt use a simple fireball model to explain the slow rise of the ratio RA≡〈NA〉/〈NN〉 of the charged multiplicity for proton-nucleus scattering to that for proton-proton scattering verses the apparent nuclear thickness <span style="border-top: 1px solid; padding-top: 0px;"><em>v</em></span>. The pseudo-rapidity distribution dNA/dη is also discussed. In this model, the pi mesons are emitted by fireballs created during nucleon-nucleon scattering. When the incident energy Elab Z 50 GeV/c2, these fire-balls take so long a time to expend to thermal equilibrium that the fireballs have passed through the nucleus completely before pions are emitted. As a result, the charged multiplicity is greatly reduced.This model gives excellent fittings to pp charged mutiplicity, RA verses <span style="border-top: 1px solid; padding-top: 0px;"><em>v</em></span> as well as Remalsion verses Elab without any free theoretical parameter. By choosing only one parameter for the equilibrium of angular momentum, dNA/dη can be fitted satisfactorily except for the large pseudo-rapidity region.
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  • [1] W. Busza, in High Energy Physics and Nuclear B'Eructure, 1975, Proc. of the 6th Inter. Conf Santa Fo and Los Alemns. edited by D. E. Nacle et al..(AIP. New York, 1975) .[2] W. Busza et al.. In Proc. of the XVIII Intor. Conf. on Hing Energy Physics. Tbilisi. 1976 edited by N. N. Bogaliubow et al (JINR, Dnbna, U. S. S. R., 1977).[3] E.Fermi, Prog. Thaor. Phys., 5(1950), 570.[4] E.Feitni. Phys. Rev., 81(1951). 683.[5] T.C. Mangy, Phys. Rev., D9(1974), 3062.[6] M. E. Law et al., Lawroneo Berkeley Laboratory No. LBL-80, 1972 (unpublished).[7] G. Bialkowski, C. B. Chiw and D. M. Tow, Phys. Rev., D17(1978), 862.[8] K. Gott.friod, Phys. Rev. Lett., 32(1974), 957.
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Get Citation
WU JING-YUAN and XIE YI-CHENG. PROTON-NUCLEUS SCATTERING IN A THERMODYNAMICAL FIREBALL MODEL[J]. Chinese Physics C, 1981, 5(1): 29-38.
WU JING-YUAN and XIE YI-CHENG. PROTON-NUCLEUS SCATTERING IN A THERMODYNAMICAL FIREBALL MODEL[J]. Chinese Physics C, 1981, 5(1): 29-38. shu
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Received: 1979-08-29
Revised: 1900-01-01
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PROTON-NUCLEUS SCATTERING IN A THERMODYNAMICAL FIREBALL MODEL

Abstract: We attempt use a simple fireball model to explain the slow rise of the ratio RA≡〈NA〉/〈NN〉 of the charged multiplicity for proton-nucleus scattering to that for proton-proton scattering verses the apparent nuclear thickness <span style="border-top: 1px solid; padding-top: 0px;"><em>v</em></span>. The pseudo-rapidity distribution dNA/dη is also discussed. In this model, the pi mesons are emitted by fireballs created during nucleon-nucleon scattering. When the incident energy Elab Z 50 GeV/c2, these fire-balls take so long a time to expend to thermal equilibrium that the fireballs have passed through the nucleus completely before pions are emitted. As a result, the charged multiplicity is greatly reduced.This model gives excellent fittings to pp charged mutiplicity, RA verses <span style="border-top: 1px solid; padding-top: 0px;"><em>v</em></span> as well as Remalsion verses Elab without any free theoretical parameter. By choosing only one parameter for the equilibrium of angular momentum, dNA/dη can be fitted satisfactorily except for the large pseudo-rapidity region.

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