Some Formulas for Invariant Phases of Unitary Matrices by Jarlskog
نویسنده
چکیده
CP violation is expected in the standard model of particle physics with three or more families [1], [2]. Therefore it is an important problem that what is the measure of CP violation with such families which is invariant under the action of phase factors. To construct invariants for matrix action, the determinant is a useful tool. In the previous paper [3], C. Jarlskog succeeded to define invariants of CP violation by using the determinant for commutator of the quark mass matrices. For the case of 3 families, it is relatively easy to calculate it. Moreover, in that case, her determinant is propotional to an invariant phase of unitary matrices. Then she discussed invariant quantities for 4 families by using projection operators and the trace of some matrices, but she did not deal with her determinant itself for n = 4 [4]. Therefore the problem is still remained. An approach to this problem is to use a parametrization for
منابع مشابه
Volume of the set of unistochastic matrices of order 3 and the mean Jarlskog invariant
A bistochastic matrix B of size N is called unistochastic if there exists a unitary U such that Bij = Uij 2 for i , j=1, . . . ,N. The set U3 of all unistochastic matrices of order N=3 forms a proper subset of the Birkhoff polytope, which contains all bistochastic doubly stochastic matrices. We compute the volume of the set U3 with respect to the flat Lebesgue measure and analytically evaluate ...
متن کاملar X iv : 0 90 9 . 01 16 v 1 [ m at h - ph ] 1 S ep 2 00 9 Volume of the set of unistochastic matrices of order 3 and the mean Jarlskog invariant
A bistochastic matrix B of size N is called unistochastic if there exists a uni-tary U such that B ij = |U ij | 2 for i, j = 1,. .. , N. The set U 3 of all unistochastic matrices of order N = 3 forms a proper subset of the Birkhoff polytope, which contains all bistochastic (doubly stochastic) matrices. We compute the volume of the set U 3 with respect to the flat (Lebesgue) measure and analytic...
متن کاملLeptogenesis and a Jarlskog Invariant
The relation between low energy CP violating phases, and the CP asymmetry of leptogenesis ǫ1, is investigated. Although it is known that in general those are independent, there may be a relation when a model is specified. We construct a Jarlskog invariant which is proportional to ǫ1 if the right-handed neutrino masses are hierarchical. Since the invariant can be expressed in terms of left-hande...
متن کاملFurther results on discrete unitary invariance
In arXiv:1607.06679, Marcus proved that certain functions of multiple matrices, when summed over the symmetries of the cube, decompose into functions of the original matrices. In this note, we generalize the results from the Marcus paper to a larger class of functions of multiple matrices. We also answer a problem posed in the Marcus paper. Marcus [1] exhibited certain functions that take multi...
متن کاملTetra-maximal Neutrino Mixing and Its Implications on Neutrino Oscillations and Collider Signatures
We propose a novel neutrino mixing pattern in terms of only two small integers 1 and 2 together with their square roots and the imaginary number i. This ansatz is referred to as the “tetra-maximal” mixing because it can be expressed as a product of four rotation matrices, whose mixing angles are all π/4 in the complex plane. It predicts θ12 = arctan(2 − √ 2) ≈ 30.4, θ13 = arcsin[( √ 2 − 1)/(2 √...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2009