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Characteristics of hardron‐nucleus interactions at 100 GeV/c

W.S. Toothacker, J. Whitmore, P.A. Elcombe, J. C. Hill, W.W. Neale, W. Kowald, W. D. Walker, Peter W. Lucas, L. Voyvodic, R. Ammar, D. Coppage, R. Davis, J. Gress, S. G. Kanekal, N. Kwak, J.M. Bishop, N. N. Biswas, N. M. Cason, V. P. Kenney, M.C.K. Mattingly, R. Ruchti, W. D. Shepard, S.J.Y. Ting

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Abstract

We report on 100 GeV/c interactions of p and p̄ with Ag and Au targets. This is a subset of the data from Fermilab experiment E597 and was performed with the 30‐inch bubble chamber and Downstream Particle Identifier. Final state protons with laboratory momentum less than 1.4 GeV/c have been identified by their ionization in the bubble chamber. Final state protons/antiprotons with laboratory momentum greater than 10 GeV/c have been identified using CRISIS, an ionization sampling drift chamber. The cross section and mean transverse momentum squared of the leading baryon from the reactions p+(Ag,Au)→p+X and p̄+(Ag,Au)→p̄+X are presented as a function of the rapidity loss of the leading baryon. The laboratory rapidity and transverse momentum squared of the associated pions are also presented.

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What this paper is about

We report on 100 GeV/c interactions of p and p̄ with Ag and Au targets. This is a subset of the data from Fermilab experiment E597 and was performed with the 30‐inch bubble chamber and Downstream Particle Identifier. Final state protons with laboratory momentum less than 1.4 GeV/c have been identified by their ionization in the bubble chamber. Final state protons/antiprotons with laboratory momentum greater than 10 GeV/c have been identified using CRISIS, an ionization sampling drift chamber. The cross section and mean transverse momentum squared of the leading baryon from the reactions p+(Ag,Au)→p+X and p̄+(Ag,Au)→p̄+X are presented as a function of the rapidity loss of the leading baryon. The laboratory rapidity and transverse momentum squared of the associated pions are also presented.

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Available abstract

We report on 100 GeV/c interactions of p and p̄ with Ag and Au targets. This is a subset of the data from Fermilab experiment E597 and was performed with the 30‐inch bubble chamber and Downstream Particle Identifier. Final state protons with laboratory momentum less than 1.4 GeV/c have been identified by their ionization in the bubble chamber. Final state protons/antiprotons with laboratory momentum greater than 10 GeV/c have been identified using CRISIS, an ionization sampling drift chamber. The cross section and mean transverse momentum squared of the leading baryon from the reactions p+(Ag,Au)→p+X and p̄+(Ag,Au)→p̄+X are presented as a function of the rapidity loss of the leading baryon. The laboratory rapidity and transverse momentum squared of the associated pions are also presented.

Key concepts: Physics, Bubble chamber, Antiproton, Nuclear physics, Pion, Baryon, Rapidity, Momentum (technical analysis)

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