2015
DOI: 10.1103/physrevd.92.053008
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Dark matter at the LHC: Effective field theories and gauge invariance

Abstract: Effective field theory (EFT) formulations of dark matter interactions have proven to be a convenient and popular way to quantify LHC bounds on dark matter. However, some of the nonrenormalizable EFT operators considered do not respect the gauge symmetries of the Standard Model. We carefully discuss under what circumstances such operators can arise, and outline potential issues in their interpretation and application. PACS numbers: 95.35.+d, 12.15.Lk

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Cited by 63 publications
(78 citation statements)
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“…As the abundance is inversely proportional to hσvi, an upper limit on the astrophysical flux can be used to set a lower limit on hσvi [see Eq. (19)]. If WIMPs make up only part of the DM mass budget, its cross section is no longer restricted to be thermal.…”
Section: Invisibles and Subdominant Densitymentioning
confidence: 99%
“…As the abundance is inversely proportional to hσvi, an upper limit on the astrophysical flux can be used to set a lower limit on hσvi [see Eq. (19)]. If WIMPs make up only part of the DM mass budget, its cross section is no longer restricted to be thermal.…”
Section: Invisibles and Subdominant Densitymentioning
confidence: 99%
“…[50][51][52] pointed out a violation of unitarity in the mono-W scattering cross section as a consequence of the lack of gauge invariance. Nevertheless, scattering processes in DD experiments involve energy scales considerably smaller than the EWSB scale, and the potential lack of electroweak gauge invariance is not a concern.…”
Section: Jhep08(2016)111mentioning
confidence: 99%
“…At the LHC CM energy, one has to respect the full SM gauge symmetry, and not just the unbroken subgroup of it. Recently, importance of the full SM invariance, unitarity and gauge invariance with respect to the mediators was noticed in a few independent studies [13][14][15], which will be detailed in the subsequent discussions. When we impose the full SM gauge symmetry, we have to realize that the SM fermions have two independent chiralities, left-handed (LH) and right-handed (RH), and SM gauge interactions are chiral as well.…”
Section: Jhep01(2017)086mentioning
confidence: 99%