The decay b→sγ and the charged Higgs boson mass bounds in a supersymmetric model without R-parity

2000 ◽  
Vol 81 ◽  
pp. 254-258
Author(s):  
E. Torrente-Lujan
1991 ◽  
Vol 271 (1-2) ◽  
pp. 123-132 ◽  
Author(s):  
Andrea Brignole ◽  
John Ellis ◽  
Giovanni Ridolfi ◽  
Fabio Zwirner

2013 ◽  
Vol 88 (5) ◽  
Author(s):  
M. Frank ◽  
L. Galeta ◽  
T. Hahn ◽  
S. Heinemeyer ◽  
W. Hollik ◽  
...  

1997 ◽  
Vol 12 (30) ◽  
pp. 2229-2236
Author(s):  
Sin Kyu Kang

We compute the charged Higgs boson mass in the minimal GMSB model. We find that the present experimental bounds on Br (b→ sγ) lead to mH±≳ 445 (686) GeV for tan β=3 (40) and Mt=175 GeV. The predictions of mH± imply that the decay mode t→ H+b is closed in the minimal GMSB model.


2008 ◽  
Vol 183 ◽  
pp. 86-90
Author(s):  
T. Hahn ◽  
S. Heinemeyer ◽  
W. Hollik ◽  
H. Rzehak ◽  
G. Weiglein

2021 ◽  
Vol 81 (1) ◽  
Author(s):  
Junxing Pan ◽  
Jung-Hsin Chen ◽  
Xiao-Gang He ◽  
Gang Li ◽  
Jhih-Ying Su

AbstractIn this work, we study the potential of searching for triply charged Higgs boson originating from a complex Higgs quadruplet in the final state with at least three same-sign leptons. A detailed collider analysis of the SM backgrounds and signals is performed at a 100 TeV pp collider for the triply charged Higgs boson mass below 1 TeV and the Higgs quadruplet vacuum expectation value $$v_\Delta $$ v Δ ranging from $$1.5\times 10^{-9}~\text {GeV}$$ 1.5 × 10 - 9 GeV to $$1.3~\text {GeV}$$ 1.3 GeV and the mass splitting $$\Delta m$$ Δ m between the nearby states of the Higgs quadruplet satisfying $$|\Delta m|\lesssim 30~\text {GeV}$$ | Δ m | ≲ 30 GeV . About $$100~\text {fb}^{-1}$$ 100 fb - 1 of data are required at most for $$5\sigma $$ 5 σ discovery. We also revisit the sensitivity at the Large Hadron Collider (LHC) and find that $$5\sigma $$ 5 σ discovery of the triply charged Higgs boson below 1 TeV can be reached for a relatively small $$v_\Delta $$ v Δ . For example, if $$v_\Delta =10^{-6}~\text {GeV}$$ v Δ = 10 - 6 GeV and $$\Delta m=0$$ Δ m = 0 , the integrated luminosity of $$330~\text {fb}^{-1}$$ 330 fb - 1 is needed. But for a relatively large $$v_\Delta $$ v Δ , i.e., $$v_\Delta \gtrsim 10^{-3}~\text {GeV}$$ v Δ ≳ 10 - 3 GeV , the triply charged Higgs boson above about 800 GeV cannot be discovered even in the high-luminosity LHC era. For $$\Delta m>0$$ Δ m > 0 , the cascade decays are open and the sensitivity can be improved depending on the value of $$v_\Delta $$ v Δ .


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