2014
DOI: 10.1007/jhep05(2014)002
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Constraints on a very light sbottom

Abstract: Abstract:We investigate the phenomenological viability of a very light bottom squark, with a mass less than half of the Z boson mass. The decays of the Z and Higgs bosons to light sbottom pairs are, in a fairly model independent manner, strongly constrained by the precision electroweak data and Higgs signal strength measurements, respectively. These constraints are complementary to direct collider searches, which depend in detail on assumptions regarding the superpartner spectrum and decays of the sbottom. In … Show more

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Cited by 11 publications
(13 citation statements)
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References 93 publications
(114 reference statements)
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“…We do not consider rare Higgs decays to SM particles, which can be very sensitive to new physics, whether through its effects in loops (such as in γγ or Zγ), through its modifications of the V-V-H couplings [41] or its nonstandard flavor structures (as in lepton family number-violating decays h → τμ; see [42,43], and references therein). (iii) The initial exotic 125 GeV Higgs decay is to two neutral BSM particles.-Generally, to compete with the SM decay modes, the Higgs decay to exotic particles needs to begin as a two-body decay, and LEP limits place stringent constraints on light charged particles [44,45]. Three-body or higher-body exotic decays typically require new states with masses m ≲ m h that have substantial couplings to the Higgs boson, in order to induce any appreciable BSM branching fraction after the phase space suppression [46].…”
Section: B Exotic-decay Modes Of the 125 Gev Higgs Bosonmentioning
confidence: 99%
“…We do not consider rare Higgs decays to SM particles, which can be very sensitive to new physics, whether through its effects in loops (such as in γγ or Zγ), through its modifications of the V-V-H couplings [41] or its nonstandard flavor structures (as in lepton family number-violating decays h → τμ; see [42,43], and references therein). (iii) The initial exotic 125 GeV Higgs decay is to two neutral BSM particles.-Generally, to compete with the SM decay modes, the Higgs decay to exotic particles needs to begin as a two-body decay, and LEP limits place stringent constraints on light charged particles [44,45]. Three-body or higher-body exotic decays typically require new states with masses m ≲ m h that have substantial couplings to the Higgs boson, in order to induce any appreciable BSM branching fraction after the phase space suppression [46].…”
Section: B Exotic-decay Modes Of the 125 Gev Higgs Bosonmentioning
confidence: 99%
“…If the R-hadron, on the other hand, is quasi-stable and is charged (CHArged Massive Particle CHAMP), it could lead to a soft charged track in the detector. Searching for such signals is interesting, but typically challenging at the LHC [180]. On the other hand, such a light and long-live charged R-hadron has been excluded by CHAMP searches at the LEP [181][182][183][184].…”
Section: Jhep08(2014)093mentioning
confidence: 99%
“…We use the FEYNHIGGS 2.11.2 [25] to calculate the MSSM Higgs mass (for an estimation of hierarchical stops twoloop contribution, see Eq. (5.3) of [26]), then solve for the X t values which are consistent with a SM like Higgs mass of 122-128 GeV.…”
mentioning
confidence: 99%