Measurement of the branching ratio and asymmetry parameter for theΣ+→pγ radiative decay

1995 ◽  
Vol 51 (9) ◽  
pp. 4638-4660 ◽  
Author(s):  
S. Timm ◽  
I. F. Albuquerque ◽  
N. F. Bondar ◽  
R. Carrigan ◽  
D. Chen ◽  
...  
2011 ◽  
Vol 26 (32) ◽  
pp. 5349-5368 ◽  
Author(s):  
I. CORTÉS-MALDONADO ◽  
G. TAVARES-VELASCO

In the little Higgs model with T-parity (LHTM), the only tree-level kinematically allowed two-body decay of the ZH boson can be the ZH→AHH decay and thus one-loop induced two-body decays may have a significant rate. We study the ZH→γAH decay, which is induced at the one-loop level by a fermion triangle and is interesting as it depends on the mechanism of anomaly cancelation of the model. All the relevant two- and three-body decays of the ZH gauge boson arising at the tree-level are also calculated. We considered a small region of the parameter space where f is still allowed to be as low as 500 GeV by electroweak precision data. We analyzed the scenario of a Higgs with a mass of 120 GeV. We found that the ZH→γAH branching ratio can be of the order of a tree-level three-body decay and may be at the reach of detection at the LHC for f close to 500 GeV, but it may be difficult to detect for f = 1 TeV . There is also an scenario where the Higgs boson has an intermediate mass such that the ZH→AHH decay is closed, the ZH→γAH gets considerably enhanced and the chances of detection get a large boost.


1993 ◽  
Vol 08 (05) ◽  
pp. 399-408 ◽  
Author(s):  
L. MAHARANA ◽  
A. NATH

The radiative decay of [Formula: see text] is considered in a field theoretic quark model. It is found that the size of the baryon plays significant role and the branching ratio of the decay is highly suppressed by the order of factor 10−8.


2021 ◽  
Vol 81 (9) ◽  
Author(s):  
Duy Nguyen Tuan ◽  
Takeo Inami ◽  
Huong Do Thi

AbstractWe investigate several phenomena related to FCNCs in the $$\text {3-3-1-1}$$ 3-3-1-1 model. The sources of FCNCs at the tree-level from both the gauge and Higgs sectors are clarified. Experiments on the oscillation of mesons most stringently constrain the tree-level FCNCs. The lower bound on the new physics scale is imposed more tightly than in the previous, $$\text {M}_{\text {new}}>12 $$ M new > 12 TeV. Under this bound, the tree-level FCNCs make a negligible contribution to the $$\text {Br}(B_s \rightarrow \mu ^+ \mu ^-)$$ Br ( B s → μ + μ - ) , $$\text {Br}(B \rightarrow K^{*} \mu ^+ \mu ^-)$$ Br ( B → K ∗ μ + μ - ) and $$\text {Br}(B^{+}\rightarrow K^{+}\mu ^{+}\mu ^{-})$$ Br ( B + → K + μ + μ - ) . The branching ratio of radiative decay $$b \rightarrow s \gamma $$ b → s γ is enhanced by the ratio $$\frac{v}{u}$$ v u via diagrams with the charged Higgs mediation. In contrast, the charged currents of new gauge bosons significantly contribute to the decay process $$\mu \rightarrow e \gamma $$ μ → e γ .


1960 ◽  
Vol 16 (5) ◽  
pp. 247
Author(s):  
CHEN YEN-FA ◽  
SONG YUH

1994 ◽  
Vol 72 (6) ◽  
pp. 808-811 ◽  
Author(s):  
T. Dubbs ◽  
I. F. Albuquerque ◽  
N. F. Bondar ◽  
R. Carrigan ◽  
D. Chen ◽  
...  

1994 ◽  
Vol 09 (17) ◽  
pp. 1545-1556 ◽  
Author(s):  
Y.Y. KEUM ◽  
X.Y. PHAM

We point out that the rare decay modes [Formula: see text], [Formula: see text] could be very much enhanced, with a branching ratio around 10−6 which is some hundreds times larger than previous predictions. Its observation will determine the W boson mass with great accuracy, providing additional high precision test of the Standard Model, as well as reveal eventual deviation from the trilinear non-Abelian gauge coupling.


1989 ◽  
Author(s):  
S. Teige ◽  
A. Beretvas ◽  
A. Caracappa ◽  
T. Devlin ◽  
H. T. Diehl ◽  
...  

1994 ◽  
Vol 50 (1) ◽  
pp. R18-R20 ◽  
Author(s):  
I. F. Albuquerque@f ◽  
N. F. Bondar@f ◽  
R. Carrigan ◽  
D. Chen ◽  
P. S. Cooper@f ◽  
...  

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