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Impact parameter representation of the leading proton spectrum in the diffractive region

Recent experiment indicates that there is no limiting value for the pion invariant inclusive cross section at x=0 at the highest energies reached by the CERN intersecting storage rings. The author first notes that a recently proposed integral representation of the leading proton spectrum is physical...

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Detalles Bibliográficos
Autor principal: Barshay, S
Lenguaje:eng
Publicado: 1975
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(75)90157-4
http://cds.cern.ch/record/873180
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author Barshay, S
author_facet Barshay, S
author_sort Barshay, S
collection CERN
description Recent experiment indicates that there is no limiting value for the pion invariant inclusive cross section at x=0 at the highest energies reached by the CERN intersecting storage rings. The author first notes that a recently proposed integral representation of the leading proton spectrum is physically equivalent to representing this spectrum in terms of very narrow multiplicity distributions from each initial impact parameter, with a single factorizable function for the average multiplicity at any impact parameter b, (n(s, b/R(s)))=N(s)n(b/R(s)). He then observes that, in this approach, the explicit form for the scaled part of the spectrum for mod x mod <0.97 and p/sub T/ approximately 0 depends essentially upon the assumed asymptotic form for the growth of average multiplicity with energy s. The data do not exclude the empirical possibility of N(s varies as s/sup epsilon /, epsilon <1/4. (19 refs).
id cern-873180
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1975
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spelling cern-8731802019-09-30T06:29:59Zdoi:10.1016/0370-2693(75)90157-4http://cds.cern.ch/record/873180engBarshay, SImpact parameter representation of the leading proton spectrum in the diffractive regionParticle Physics - PhenomenologyRecent experiment indicates that there is no limiting value for the pion invariant inclusive cross section at x=0 at the highest energies reached by the CERN intersecting storage rings. The author first notes that a recently proposed integral representation of the leading proton spectrum is physically equivalent to representing this spectrum in terms of very narrow multiplicity distributions from each initial impact parameter, with a single factorizable function for the average multiplicity at any impact parameter b, (n(s, b/R(s)))=N(s)n(b/R(s)). He then observes that, in this approach, the explicit form for the scaled part of the spectrum for mod x mod <0.97 and p/sub T/ approximately 0 depends essentially upon the assumed asymptotic form for the growth of average multiplicity with energy s. The data do not exclude the empirical possibility of N(s varies as s/sup epsilon /, epsilon <1/4. (19 refs).oai:cds.cern.ch:8731801975
spellingShingle Particle Physics - Phenomenology
Barshay, S
Impact parameter representation of the leading proton spectrum in the diffractive region
title Impact parameter representation of the leading proton spectrum in the diffractive region
title_full Impact parameter representation of the leading proton spectrum in the diffractive region
title_fullStr Impact parameter representation of the leading proton spectrum in the diffractive region
title_full_unstemmed Impact parameter representation of the leading proton spectrum in the diffractive region
title_short Impact parameter representation of the leading proton spectrum in the diffractive region
title_sort impact parameter representation of the leading proton spectrum in the diffractive region
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(75)90157-4
http://cds.cern.ch/record/873180
work_keys_str_mv AT barshays impactparameterrepresentationoftheleadingprotonspectruminthediffractiveregion