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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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Lenguaje: | eng |
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1975
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(75)90157-4 http://cds.cern.ch/record/873180 |
_version_ | 1780907646995398656 |
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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 |
record_format | invenio |
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 |