It has been shown that QED in (1+4)-dimensional space-time, with the fifth dimension compactified on a circle, leads to CP violation (CPV). Depending on fermionic boundary conditions, CPV may be either explicit (through the Scherk--Schwarz mechanism), or spontaneous (via the Hosotani mechanism). The fifth component of the gauge field acquires (at the one-loop level) a non-zero vacuum expectation value. In the presence of two fermionic fields, this leads to spontaneous CPV in the case of CP-symmetric boundary conditions. Phenomenological consequences are illustrated by a calculation of the electric dipole moment for the fermionic zero-modes
AbstractQCD in a five-dimensional sliced bulk with chiral extra-quarks on the boundaries is generica...
The CP transformation combines charge conjugation C with parity P. Under C, particles and antipartic...
We investigate (2 + 1)-dimensional QED coupled with Dirac fermions both at zero and finite temperatu...
One of the Sakharov's condition for baryogenesis is the violation of both C and CP. In the Standard ...
[[abstract]]We construct a realistic model of CP violation in which CP is broken in the process of d...
[[abstract]]We give a new configuration of split fermion positions in one extra dimension with two d...
We put forward the conjecture that all CP violating phenomena may have a common origin. In order to ...
We study spontaneous CP violation as a solution to the strong CP problem in left-right symmetric the...
Electric dipole moments (EDMs) break parity (P) and time-reversal (T) symmetry and thus, by the CPT ...
The Strong CP Problem is the contradiction between the experimental evidence and the existence of a ...
In this paper, we examine the CP-violating term of the Euler–Heisenberg action. We focus in the aspe...
We propose a new mechanism to generate a CP phase originating from a non-trivial Higgs vacuum expect...
We study how to incorporate CP violation in the Froggatt--Nielsen (FN) mechanism. To this end, we in...
We introduce a CP symmetric model where masses of fermions are given by dimensional-5 operators, and...
We consider quantum effects in a world with two coexisting symmetry phases, unbroken and spontaneous...
AbstractQCD in a five-dimensional sliced bulk with chiral extra-quarks on the boundaries is generica...
The CP transformation combines charge conjugation C with parity P. Under C, particles and antipartic...
We investigate (2 + 1)-dimensional QED coupled with Dirac fermions both at zero and finite temperatu...
One of the Sakharov's condition for baryogenesis is the violation of both C and CP. In the Standard ...
[[abstract]]We construct a realistic model of CP violation in which CP is broken in the process of d...
[[abstract]]We give a new configuration of split fermion positions in one extra dimension with two d...
We put forward the conjecture that all CP violating phenomena may have a common origin. In order to ...
We study spontaneous CP violation as a solution to the strong CP problem in left-right symmetric the...
Electric dipole moments (EDMs) break parity (P) and time-reversal (T) symmetry and thus, by the CPT ...
The Strong CP Problem is the contradiction between the experimental evidence and the existence of a ...
In this paper, we examine the CP-violating term of the Euler–Heisenberg action. We focus in the aspe...
We propose a new mechanism to generate a CP phase originating from a non-trivial Higgs vacuum expect...
We study how to incorporate CP violation in the Froggatt--Nielsen (FN) mechanism. To this end, we in...
We introduce a CP symmetric model where masses of fermions are given by dimensional-5 operators, and...
We consider quantum effects in a world with two coexisting symmetry phases, unbroken and spontaneous...
AbstractQCD in a five-dimensional sliced bulk with chiral extra-quarks on the boundaries is generica...
The CP transformation combines charge conjugation C with parity P. Under C, particles and antipartic...
We investigate (2 + 1)-dimensional QED coupled with Dirac fermions both at zero and finite temperatu...