Multiparticle production in the large lambda n limit: Realising Higgsplosion in a scalar QFT
arXiv:1705.04365 · doi:10.1007/JHEP06(2017)148
Abstract
In a scalar theory which we use as a simplified model for the Higgs sector, we adopt the semiclassical formalism of Son for computations of -particle production cross-sections in the high-multiplicity weak-coupling regime with the value of held fixed and large. The approach relies on the use of singular classical solutions to a certain boundary value problem. In the past this formalism has been successfully used and verified in computations of perturbative multi-particle processes at tree-level, and also at the next-to-leading order level in the small expansion near the multi-particle mass threshold. We apply this singular solutions formalism in the regime of ultra-high multiplicities where , and compute the leading positive contribution to the exponent of the multi-particle rate in this large limit. The computation is carried out near the multi-particle mass threshold where the multiplicity approaches its maximal value allowed by kinematics. This calculation relies on the idea of Gorsky and Voloshin to use a thin wall approximation for the singular solutions that resemble critical bubbles. This approximation is justified in precisely the high-multiplicity regime of interest. Based on our results we show that the scalar theory with a spontaneous symmetry breaking used here as a simplified model for the Higgs sector, is very likely to realise the high-energy Higgsplosion phenomenon.
21 pages, 2 figures, v2: minor corrections, matches version accepted in JHEP, v3: extended discussion below Eq. (4.10), minor corrections, v4: few typos (signs and factors) corrected in intermediate results
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