Abstract

A $6.8 \ {\rm nb^{-1}}$ sample of $pp$ collision data collected under low-luminosity conditions at $\sqrt{s} = 7$ TeV by the ATLAS detector at the Large Hadron Collider is used to study diffractive dijet production. Events containing at least two jets with $p_\mathrm{T} > 20$ GeV are selected and analysed in terms of variables which discriminate between diffractive and non-diffractive processes. Cross sections are measured differentially in $\Delta\eta^F$, the size of the observable forward region of pseudorapidity which is devoid of hadronic activity, and in an estimator, $\tilde{\xi}$, of the fractional momentum loss of the proton assuming single diffractive dissociation ($pp \rightarrow pX$). Model comparisons indicate a dominant non-diffractive contribution up to moderately large $\Delta\eta^F$ and small $\tilde{\xi}$, with a diffractive contribution which is significant at the highest $\Delta\eta^F$ and the lowest $\tilde{\xi}$. The rapidity-gap survival probability is estimated from comparisons of the data in this latter region with predictions based on diffractive parton distribution functions.

Highlights

  • Diffractive dissociation contributes a large fraction of the total inelastic cross section [1] at the Large Hadron Collider (LHC)

  • The total resulting uncertainty in the differential cross sections measured here varies from 20% for small gaps to ∼40% for very large gaps, a region which is dominated by diffractive events with relatively small transverse momentum or large pseudorapidity of jets

  • An ATLAS measurement of the cross section for dijet production in association with forward rapidity gaps is reported, based on 6.8 nb−1 low pile-up 7 TeV pp collision data taken at the LHC in 2010

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Summary

Introduction

Diffractive dissociation (e.g. pp → p X ) contributes a large fraction of the total inelastic cross section [1] at the Large Hadron Collider (LHC). A similar ‘rapidity-gap survival probability’ factor, usually denoted by S2, was suggested by the first results from the LHC [15] This factorisation breaking is usually attributed to secondary scattering from beam remnants, referred to as absorptive corrections, and closely related to the multiple-scattering effects which are a primary focus of underlying-event studies [16,17,18]. Understanding these effects more deeply is an important step towards a complete model of diffractive processes at hadronic colliders and may point the way towards a reconciliation of the currently very different theoretical treatments of soft and hard strong interactions. Comparisons between the measurements and the predictions provide estimates of the rapidity-gap survival probability applicable to single dissociation processes at LHC energies

Models and simulations
The ATLAS detector
Experimental method
Systematic uncertainties
Results
Conclusions
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