1986
DOI: 10.1103/physrevd.33.755
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Two-photon decays of scalar and pseudoscalar bosons in supersymmetry

Abstract: We calculate the one-loop contribution to the two-photon decay widths of scalar and pseudoscalar bosons in a supersymmetric SU(2)XU( 1) gauge theory using component fields. Effective Lagrangians for these reactions are also constructed using superfields, thus confirming that these widths do not vanish in the supersymmetric limit.

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Cited by 27 publications
(27 citation statements)
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“…What can still deviate, is the strength of the hγ γ interaction. This is attributed to the participation of the charged Higgs in the loop [32,[52][53][54][55]. The corresponding decay width is given by…”
Section: Higgs Signal Strengthsmentioning
confidence: 99%
“…What can still deviate, is the strength of the hγ γ interaction. This is attributed to the participation of the charged Higgs in the loop [32,[52][53][54][55]. The corresponding decay width is given by…”
Section: Higgs Signal Strengthsmentioning
confidence: 99%
“…Let us note that in our model the Higgs-top quark coupling is very close to the SM expectation, i.e., a htt 1, since the mixing between the CP even neutral scalar fields ξ η and ξ χ is very suppressed, being the 126 GeV SM like Higgs boson mainly composed of the ξ η field. The dimensionless loop factors F 1/2 (ρ) and F 1 (ρ) for spin-1/2 and spin-1 particles in the loop, respectively are [190][191][192][193][194][195][196][197]:…”
Section: Higgs Diphoton Ratementioning
confidence: 99%
“…yy a n d Z Z decays of Higgs b o s o~i s i n SUSY e v e n t s T h e yy and Z Z decays of tlie MSShl Higgs h o s o~l s lead t o a prornisi~ig riiethod for their ide~itificatiori a t I i a t l r o~~ colliders [16,24]. It is therefore natural t o study whether one can see these decay modes for Higgs bosons produced in SUSY events.…”
Section: B T Multiplicity In Susy Eventsmentioning
confidence: 99%
“…This is not surprising since, as discussed in Ref. (161, the contribution of the t-quark loop t o H , decay is strongly suppressed when t a n P is substantially larger than unity. This is essentially t h e reason why H p -+ yy signals are observable only when t a n p is close t o unity [16,24]. Since t a n @ = 1 maximizes this decay (remember we d o not allow for t a n p < I ) , we have computed this branching fraction for t h e smallest value of mH+ (162 GeV) allowed by Fig.…”
Section: B T Multiplicity In Susy Eventsmentioning
confidence: 99%