Study of Discrete Symmetries for $$B_s$$ Meson System

Author(s):  
Bharti Kindra ◽  
Namit Mahajan
2016 ◽  
Vol 902 ◽  
pp. 1-57 ◽  
Author(s):  
I. Girardi ◽  
S.T. Petcov ◽  
Alexander J. Stuart ◽  
A.V. Titov

2021 ◽  
Vol 103 (10) ◽  
Author(s):  
Michele Arzano ◽  
Andrea Bevilacqua ◽  
Jerzy Kowalski-Glikman ◽  
Giacomo Rosati ◽  
Josua Unger
Keyword(s):  

1995 ◽  
Author(s):  
B. M. K. Nefkens
Keyword(s):  

1989 ◽  
Vol 232 (1) ◽  
pp. 104-112 ◽  
Author(s):  
D. Kapetanakis ◽  
G. Zoupanos

2008 ◽  
Vol 23 (39) ◽  
pp. 3271-3283 ◽  
Author(s):  
HYE-SUNG LEE

Supersymmetry is one of the best motivated new physics scenarios. To build a realistic supersymmetric standard model, however, a companion symmetry is necessary to address various issues. While R-parity is a popular candidate that can address the proton and dark matter issues simultaneously, it is not the only option for such a property. We review how a TeV scale U(1)′ gauge symmetry can replace the R-parity. Discrete symmetries of the U(1)′ can make the model still viable and attractive with distinguishable phenomenology. For instance, with a residual discrete symmetry of the U(1)′, Z6 = B3 × U2, the proton can be protected by the baryon triality (B3) and a hidden sector dark matter candidate can be protected by the U-parity (U2).


2013 ◽  
Vol 877 (3) ◽  
pp. 752-771 ◽  
Author(s):  
Stefan Antusch ◽  
Martin Holthausen ◽  
Michael A. Schmidt ◽  
Martin Spinrath

1978 ◽  
Vol 74 (4-5) ◽  
pp. 344-346 ◽  
Author(s):  
R. Barbieri ◽  
R. Gatto ◽  
F. Strocchi

2014 ◽  
Vol 29 (32) ◽  
pp. 1450173 ◽  
Author(s):  
D. Cogollo ◽  
Farinaldo S. Queiroz ◽  
P. Vasconcelos

In this work, we overhaul previous studies of Flavor Changing Neutral Current processes in the context of the Reduced Minimal 3-3-1 (RM331) model. We sift the individual contributions from the CP-even scalars and the Z′ gauge boson using two different parametrizations schemes and compare our results with current measurements. In particular, studying the [Formula: see text] meson system we find the most stringent bounds in the literature on this model, namely [Formula: see text] and [Formula: see text].


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