scholarly journals R-parity violation and quark flavor violation

1997 ◽  
Vol 55 (7) ◽  
pp. 4222-4239 ◽  
Author(s):  
B. de Carlos ◽  
P. L. White
2015 ◽  
Vol 91 (1) ◽  
Author(s):  
A. Bartl ◽  
H. Eberl ◽  
E. Ginina ◽  
K. Hidaka ◽  
W. Majerotto

2015 ◽  
Vol 2015 ◽  
pp. 1-22 ◽  
Author(s):  
A. Vicente

Most extensions of the Standard Model lepton sector predict large lepton flavor violating rates. Given the promising experimental perspectives for lepton flavor violation in the next few years, this generic expectation might offer a powerful indirect probe to look for new physics. In this review we will cover several aspects of lepton flavor violation in supersymmetric models beyond the Minimal Supersymmetric Standard Model. In particular, we will concentrate on three different scenarios: high-scale and low-scale seesaw models as well as models withR-parity violation. We will see that in some cases the LFV phenomenology can have characteristic features for specific scenarios, implying that dedicated studies must be performed in order to correctly understand the phenomenology in nonminimal supersymmetric models.


2015 ◽  
Vol 30 (15) ◽  
pp. 1540013 ◽  
Author(s):  
Gero von Gersdorff

We review constraints from quark and lepton flavor violation on extra dimensional models with warped geometry, both in the minimal and the custodial model. For both scenarios, Kaluza–Klein (KK) masses that are large enough to suppress constraints from electroweak precision tests (EWPT) also sufficiently suppress all quark flavor and CP violation, with the exception of CP violation in [Formula: see text] mixing and (to a lesser extend) in [Formula: see text] mixing. In the lepton sector the minimal scenario leads to excessively large contributions to μ→eγ transitions, requiring KK masses of at least 20 TeV or larger.


2014 ◽  
Vol 29 (07) ◽  
pp. 1450035 ◽  
Author(s):  
A. Bartl ◽  
H. Eberl ◽  
E. Ginina ◽  
B. Herrmann ◽  
K. Hidaka ◽  
...  

We study quark flavor violation (QFV) in the squark sector of the Minimal Supersymmetric Standard Model (MSSM). We assume mixing between the second and the third squark generations, i.e. [Formula: see text] mixing. We focus on QFV effects in bosonic squark decays, in particular on the decay into the lightest Higgs boson [Formula: see text], where [Formula: see text] are the lightest up-type squarks. We show that the branching ratio of this QFV decay can be quite large (up to 50%) due to large QFV trilinear couplings, and large [Formula: see text] and [Formula: see text] mixing, despite the strong constraints on QFV from B meson data. This can result in characteristic QFV final states with significant rates at LHC (14 TeV), such as [Formula: see text] and [Formula: see text]. The QFV bosonic squark decays can have an influence on the squark and gluino searches at LHC.


2000 ◽  
Vol 488 (2) ◽  
pp. 145-152 ◽  
Author(s):  
Kiwoon Choi ◽  
Eung Jin Chun ◽  
Kyuwan Hwang

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