scholarly journals The CKM phase and $$ \overline{\theta} $$ in Nelson-Barr models

2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Alessandro Valenti ◽  
Luca Vecchi

Abstract We analyze the Nelson-Barr approach to the Strong CP Problem. We derive the necessary conditions in order to simultaneously reproduce the CKM phase and the quark masses. Then we quantify the irreducible contributions to the QCD topological angle, namely the corrections arising from loops of the colored fermion mediators that characterize these models. Corrections analytic in the couplings first arise at 3-loop order and are safely below current bounds; non-analytic effects are 2-loop order and decouple as the mediators exceed a few TeV. We discuss collider, electroweak, and flavor bounds and argue that most of the parameter space above the TeV scale is still allowed in models with down-type mediators, whereas other scenarios are more severely constrained. With two or more families of mediators the dominant experimental bound is due to the neutron electric dipole moment.

2007 ◽  
Vol 22 (05) ◽  
pp. 355-366 ◽  
Author(s):  
WENJUAN ZOU ◽  
ZHENJUN XIAO

In this paper, we calculated the supersymmetric contributions to the branching ratios and CP-violating asymmetries of the four B→Kπ decays in both the general and the constrained minimal supergravity (mSUGRA) model. Within the considered parameter space, we found that (a) the phase ϕμin the general mSUGRA model is strongly constrained by the data of the electron and neutron electric dipole moment and the data of B→Xsγ decay: ϕμ<0.1 (<10-3) for the case of small (large) tan β, but no limit on the phase ϕAcan be derived from the above data; (b) in both the general and the constrained mSUGRA model, the SUSY contributions are not large enough to explain the observed B→Kπ puzzle.


1996 ◽  
Vol 11 (22) ◽  
pp. 1835-1842
Author(s):  
KEN WATANUKI ◽  
ICHIRO OHBA

The neutron electric dipole moment (EDM) is investigated in detail. We assume a phenomenologically successful seesaw-type quark mass matrix. If the neutron EDM is observed at slightly below the present experimental bound (10–26–10–25 e · cm ), we can conclude that there must exist a vector-like quark a little heavier than the heavier neutral Higgs boson, or both of them have equal masses around 1 TeV.


2021 ◽  
Vol 103 (5) ◽  
Author(s):  
C. Alexandrou ◽  
A. Athenodorou ◽  
K. Hadjiyiannakou ◽  
A. Todaro

Nature ◽  
1981 ◽  
Vol 293 (5827) ◽  
pp. 41-43 ◽  
Author(s):  
John Ellis ◽  
Mary K. Gaillard ◽  
D. V. Nanopoulos ◽  
Serge Rudaz

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