2016
DOI: 10.1140/epjc/s10052-015-3832-8
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Exclusive physics at the LHC with SuperChic 2

Abstract: We present a range of physics results for central exclusive production processes at the LHC, using the new SuperChic 2 Monte Carlo event generator. This includes significant theoretical improvements and updates, most importantly a fully differential treatment of the soft survival factor, as well as a greater number of generated processes. We provide an overview of the latest theoretical framework, and consider in detail a selection of final states, namely exclusive 2 and 3 jets, photoproduced vector mesons, tw… Show more

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Cited by 92 publications
(189 citation statements)
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References 80 publications
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“…This is in a regime where the proton optical density Ω(b t ), which is required to calculate the survival factor (see appendix A), is well constrained to be small in size. This means that any allowed variation in its value results in a very small change in the probability of no inelastic production exp(−Ω(b t )); in [49] various models for Ω(b t ) are taken for a range of photon-induced processes, and the variation in the resulting cross sections is found to be at the ∼ % level. Thus in this exclusive case the expected theoretical uncertainty is extremely small, of order a few percent.…”
Section: Jhep03(2016)182mentioning
confidence: 99%
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“…This is in a regime where the proton optical density Ω(b t ), which is required to calculate the survival factor (see appendix A), is well constrained to be small in size. This means that any allowed variation in its value results in a very small change in the probability of no inelastic production exp(−Ω(b t )); in [49] various models for Ω(b t ) are taken for a range of photon-induced processes, and the variation in the resulting cross sections is found to be at the ∼ % level. Thus in this exclusive case the expected theoretical uncertainty is extremely small, of order a few percent.…”
Section: Jhep03(2016)182mentioning
confidence: 99%
“…where V µν is the usual γγ → R vertex, see [49] for further discussion, and q i ⊥ are the photon transverse momenta. Comparing to the coupling of R to external photons, we can see that the q i ⊥ play the role of the photon polarisation vectors, which are therefore directed along their transverse momenta.…”
Section: Spin-parity Analysismentioning
confidence: 99%
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