Abstract:Radiative corrections to the decay h → Z γ are evaluated in the one-loop approximation. The unitary gauge is used. The analytic result is expressed in terms of the Passarino-Veltman functions. The calculations are applicable for the Standard Model as well for a wide class of its gauge extensions. In particular, the decay width of a charged Higgs boson H ± → W ± γ can be derived. The consistence of our formulas and several specific earlier results is shown. ening discussions and comments about divergences and c… Show more
“…In addition,G 0 = A, Z 1 , Z 2 , Z 3 belong to the linear combinations of neutral gauge bosons. Then, theLagrangian (23) is written in a standard form as follows:…”
Section: Feynman Rules For Self-couplings Of Gauge Bosonsmentioning
confidence: 99%
“…where W + ≡ W 12 is the SM charged gauge boson and X = {(12, 13), (12,14), (13,14), (13,23), (13,14), (23,24), (14,24), (14, 34), (24, 34)} Y = { (12,23), (12,24), (13, 34), (23, 34)}.…”
Feynman rules for self-couplings of the gauge bosons in the general 3-4-1 model based on the gauge group $SU(3)_c\otimes SU(4)_L \otimes U(1)_X$ will be presented in this work. The results are checked to be consistent with previous works. The results also confirm important relations between different triple and quartic gauge couplings assumed previously for constructing general one-loop contributions to physical processes searched by experiments.
“…In addition,G 0 = A, Z 1 , Z 2 , Z 3 belong to the linear combinations of neutral gauge bosons. Then, theLagrangian (23) is written in a standard form as follows:…”
Section: Feynman Rules For Self-couplings Of Gauge Bosonsmentioning
confidence: 99%
“…where W + ≡ W 12 is the SM charged gauge boson and X = {(12, 13), (12,14), (13,14), (13,23), (13,14), (23,24), (14,24), (14, 34), (24, 34)} Y = { (12,23), (12,24), (13, 34), (23, 34)}.…”
Feynman rules for self-couplings of the gauge bosons in the general 3-4-1 model based on the gauge group $SU(3)_c\otimes SU(4)_L \otimes U(1)_X$ will be presented in this work. The results are checked to be consistent with previous works. The results also confirm important relations between different triple and quartic gauge couplings assumed previously for constructing general one-loop contributions to physical processes searched by experiments.
“…While one-loop electroweak corrections to Higgs boson decay into γγ, Zγ, ZZ have been calculated in Refs. [31,32,33,34,36,37,38,39,40,41]. In this paper, we present one-loop on-shell and off-shell decays H → V V with V V = γγ, Zγ, ZZ.…”
One-loop on-shell and off-shell decays H → VV with VV = γγ, Zγ, ZZ are presented in this paper. The effects of one-loop on-shell and off-shell Higgs decays via Higgs productions at future lepton colliders are also then examined. We find that the impacts of one-loop Higgs decays are significant and they are should be taken into account at future lepton colliders.
“…While one-loop electroweak corrections to Higgs boson decay into γγ, Zγ, ZZ have been calculated in Refs. [31,32,33,34,36,37,38,39,40,41]. In this paper, we present one-loop on-shell and off-shell decays H → V V with V V = γγ, Zγ, ZZ.…”
One-loop on-shell and off-shell decays H → V V with V V = γγ, Zγ, ZZ are presented in this paper. The effects of one-loop on-shell and off-shell Higgs decays in Higgs productions at e − e − collisions are also then examined. We find that the impacts of one-loop Higgs decays are significant and they are must be taken into account at e − e − collision.
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