Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV

Pseudorapidity gap distributions in proton-proton collisions at root s = 7 TeV are studied using a minimum bias data sample with an integrated luminosity of 7.1 mu b(-1). Cross sections are measured differentially in terms of Delta eta(F), the larger of the pseudorapidity regions extending to the li...

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Main Authors: Aad, G., Brenner, Richard, Buszello, Claus P., Ekelöf, Tord, Ellert, Mattias, Ferrari, Arnaud, Isaksson, Charlie, Zwalinski, L.
Format: Others
Language:English
Published: Uppsala universitet, Högenergifysik 2012
Online Access:http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-175053
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spelling ndltd-UPSALLA1-oai-DiVA.org-uu-1750532013-07-04T04:10:07ZRapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeVengAad, G.Brenner, RichardBuszello, Claus P.Ekelöf, TordEllert, MattiasFerrari, ArnaudIsaksson, CharlieZwalinski, L.Uppsala universitet, HögenergifysikUppsala universitet, HögenergifysikUppsala universitet, HögenergifysikUppsala universitet, HögenergifysikUppsala universitet, HögenergifysikUppsala universitet, Högenergifysik2012Pseudorapidity gap distributions in proton-proton collisions at root s = 7 TeV are studied using a minimum bias data sample with an integrated luminosity of 7.1 mu b(-1). Cross sections are measured differentially in terms of Delta eta(F), the larger of the pseudorapidity regions extending to the limits of the ATLAS sensitivity, at eta = +/- 4.9, in which no final state particles are produced above a transverse momentum threshold p(T)(cut). The measurements span the region 0 &lt; Delta eta(F) &lt; 8 for 200 MeV &lt; p(T)(cut) &lt; 800 MeV. At small Delta eta(F), the data test the reliability of hadronisation models in describing rapidity and transverse momentum fluctuations in final state particle production. The measurements at larger gap sizes are dominated by contributions from the single diffractive dissociation process (pp -&gt; Xp), enhanced by double dissociation (pp -&gt; XY) where the invariant mass of the lighter of the two dissociation systems satisfies M-Y less than or similar to 7 GeV. The resulting cross section is ds sigma/d Delta eta(F) approximate to 1 mb for Delta eta(F) greater than or similar to 3. The large rapidity gap data are used to constrain the value of the Pomeron intercept appropriate to triple Regge models of soft diffraction. The cross section integrated over all gap sizes is compared with other LHC inelastic cross section measurements. <p>ATLAS Collaboration, for complete list of authors see http://dx.doi.org/10.1140/epjc/s10052-012-1926-0</p>Article in journalinfo:eu-repo/semantics/articletexthttp://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-175053doi:10.1140/epjc/s10052-012-1926-0ISI:000302540000042European Physical Journal C, 1434-6044, 2012, 72:3, s. 1926-application/pdfinfo:eu-repo/semantics/openAccess
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description Pseudorapidity gap distributions in proton-proton collisions at root s = 7 TeV are studied using a minimum bias data sample with an integrated luminosity of 7.1 mu b(-1). Cross sections are measured differentially in terms of Delta eta(F), the larger of the pseudorapidity regions extending to the limits of the ATLAS sensitivity, at eta = +/- 4.9, in which no final state particles are produced above a transverse momentum threshold p(T)(cut). The measurements span the region 0 &lt; Delta eta(F) &lt; 8 for 200 MeV &lt; p(T)(cut) &lt; 800 MeV. At small Delta eta(F), the data test the reliability of hadronisation models in describing rapidity and transverse momentum fluctuations in final state particle production. The measurements at larger gap sizes are dominated by contributions from the single diffractive dissociation process (pp -&gt; Xp), enhanced by double dissociation (pp -&gt; XY) where the invariant mass of the lighter of the two dissociation systems satisfies M-Y less than or similar to 7 GeV. The resulting cross section is ds sigma/d Delta eta(F) approximate to 1 mb for Delta eta(F) greater than or similar to 3. The large rapidity gap data are used to constrain the value of the Pomeron intercept appropriate to triple Regge models of soft diffraction. The cross section integrated over all gap sizes is compared with other LHC inelastic cross section measurements. === <p>ATLAS Collaboration, for complete list of authors see http://dx.doi.org/10.1140/epjc/s10052-012-1926-0</p>
author Aad, G.
Brenner, Richard
Buszello, Claus P.
Ekelöf, Tord
Ellert, Mattias
Ferrari, Arnaud
Isaksson, Charlie
Zwalinski, L.
spellingShingle Aad, G.
Brenner, Richard
Buszello, Claus P.
Ekelöf, Tord
Ellert, Mattias
Ferrari, Arnaud
Isaksson, Charlie
Zwalinski, L.
Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
author_facet Aad, G.
Brenner, Richard
Buszello, Claus P.
Ekelöf, Tord
Ellert, Mattias
Ferrari, Arnaud
Isaksson, Charlie
Zwalinski, L.
author_sort Aad, G.
title Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
title_short Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
title_full Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
title_fullStr Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
title_full_unstemmed Rapidity gap cross sections measured with the ATLAS detector in pp collisions at root s=7 TeV
title_sort rapidity gap cross sections measured with the atlas detector in pp collisions at root s=7 tev
publisher Uppsala universitet, Högenergifysik
publishDate 2012
url http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-175053
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