2012
DOI: 10.1140/epjc/s10052-012-1926-0
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Rapidity gap cross sections measured with the ATLAS detector in pp collisions at $\sqrt{s} = 7 \mbox{~TeV}$

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Cited by 106 publications
(56 citation statements)
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“…3 If we replace σ inel (ξ > 10 −6 ) = 67.5 ± 1.6(lumi) mb [14] by the ATLAS value of 68.1 ± 1.3(lumi) mb [13] then we find the bit smaller value of about 8 mb in (16). 4 It is also possible that the value of dσ D /dln(M 2 X ) may be a bit larger for a lower M X value, in particular due to secondary Reggeon contributions, see Fig.9 of [17].…”
Section: Real Part Of the Elastic Pp Amplitudementioning
confidence: 98%
“…3 If we replace σ inel (ξ > 10 −6 ) = 67.5 ± 1.6(lumi) mb [14] by the ATLAS value of 68.1 ± 1.3(lumi) mb [13] then we find the bit smaller value of about 8 mb in (16). 4 It is also possible that the value of dσ D /dln(M 2 X ) may be a bit larger for a lower M X value, in particular due to secondary Reggeon contributions, see Fig.9 of [17].…”
Section: Real Part Of the Elastic Pp Amplitudementioning
confidence: 98%
“…In principle the M D -distribution could be measured in pp collisions at LHC, but it is quite challenging to isolate single diffraction from the experimental distribution in the size of a gap in rapidity (see refs. [70,71]).…”
Section: Diffractively Excited Nucleonsmentioning
confidence: 99%
“…At the LHC, diffraction has been studied both by ATLAS [39][40][41] and CMS [42][43][44]. One key observation there is that the Pythia default P flux shape does not describe the rapidity gap distribution so well, suggesting that a new parametrization may be needed.…”
Section: Comparisons With Datamentioning
confidence: 99%