2015
DOI: 10.1007/jhep03(2015)162
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Heavy neutralino relic abundance with Sommerfeld enhancements — a study of pMSSM scenarios

Abstract: We present a detailed discussion of Sommerfeld enhancements in neutralino dark matter relic abundance calculations for several popular benchmark scenarios in the general MSSM. Our analysis is focused on models with heavy wino-and higgsino-like neutralino LSP and models interpolating between these two scenarios. This work is the first phenomenological application of effective field theory methods that we have developed in earlier work and that allow for the consistent study of Sommerfeld enhancements in nonrela… Show more

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Cited by 52 publications
(91 citation statements)
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“…28 in the bi-dimensional plane (m ψ 1 , σ SI ψ 1 p ). The plot shows also the current and expected limits by 38 The maximal value of the DM mass is actually higher because of Sommerfeld enhancement [352][353][354]. For simplicity we have neglected this effect since it would marginally influence the discussion.…”
Section: Majorana Dmmentioning
confidence: 90%
“…28 in the bi-dimensional plane (m ψ 1 , σ SI ψ 1 p ). The plot shows also the current and expected limits by 38 The maximal value of the DM mass is actually higher because of Sommerfeld enhancement [352][353][354]. For simplicity we have neglected this effect since it would marginally influence the discussion.…”
Section: Majorana Dmmentioning
confidence: 90%
“…We follow a general formalism developed for SUSY in ref. [24][25][26][27] to calculate absorptive Wilson coefficients and non-relativistic potentials between various two-body states, and we numerically solve resulting Schrödinger equations to obtain SRT effects.…”
Section: Jhep01(2017)009mentioning
confidence: 99%
“…Well below the threshold, SRT effects are independent on the DM velocity as the W -boson exchange in χ 0 χ 0 → χ + χ − becomes governed by the W -mass rather than the DM momentum [13,14,27], depicted as vertical regions of enhancement. The SRT effect saturates at finite enhancement in the v → 0 limit because of the finite-ranged W -exchange Yukawa potential.…”
Section: Jhep01(2017)009mentioning
confidence: 99%
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“…The effects giving rise to this are twofold. First, one has to take into account the so-called Sommerfeld effect, which is generated by the electroweak Yukawa force acting on the DM particles prior to their annihilation [13][14][15][16]. Secondly, for heavy DM annihilation into energetic particles, electroweak Sudakov (double) logarithms O((α 2 ln 2 (m χ /m W ))) are large and need to be resummed to all orders in the coupling constant [17][18][19][20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%