Possible Effects of Noncommutative Geometry on Weak CP Violation and Unitarity Triangles
نویسندگان
چکیده
Possible effects of noncommutative geometry on weak CP violation and unitarity triangles are discussed by taking account of a simple version of the momentum-dependent quark mixing matrix in the noncommutative standard model. In particular, we calculate nine rephasing invariants of CP violation and illustrate the noncommutative CP -violating effect in a couple of charged D-meson decays. We also show how inner angles of the deformed unitarity triangles are related to CP -violating asymmetries in some typical Bd and Bs transitions into CP eigenstates. B-meson factories are expected to help probe or constrain noncommutative geometry at low energies in the near future. PACS number(s): 11.90.+t, 11.30.Er, 12.60.-i Typeset using REVTEX
منابع مشابه
On the Unitarity Triangles of the CKM Matrix
The unitarity triangles of the 3 × 3 Cabibbo-Kobayashi-Maskawa (CKM) matrix are studied in a systematic way. We show that the phases of the nine CKM rephasing invariants are indeed the outer angles of the six unitarity triangles and measurable in the CP -violating decay modes of Bd and Bs mesons. An economical notation system is introduced for describing properties of the unitarity triangles. T...
متن کاملCP - violation from Noncommutative Geometry ∗
If the geometry of space-time is noncommutative, i.e. [x µ , x ν ] = iθ µν , then noncommutative CP violating effects may be manifest at low energies. For a noncommutative scale Λ ≡ θ −1/2 ≤ 2 T eV , CP violation from noncommutative geometry is comparable to that from the Standard Model (SM) alone: the noncommutative contributions to ǫ and ǫ ′ /ǫ in the K-system, and to sin 2β in the B-system, ...
متن کاملCabibbo-Kobayashi-Maskawa Matrix Unitarity Triangle and Geometry Origin of the Weak CP Phase
In this work, the postulation that weak CP phase originates in a certain geometry, is further discussed. According to this postulation, the weak CP phase is determined by three mixing angles. So, if we can determine experimentally three elements of the Cabibbo-KobayashiMaskawa (CKM) matrix, we can then determine the whole CKM matrix and correspondingly, the unitarity triangle. We find that the ...
متن کاملBuilding the full PMNS Matrix from six independent Majorana-type phases
In the framework of three light Majorana neutrinos, we show how to reconstruct, through the use of 3 × 3 unitarity, the full PMNS matrix from six independent Majorana-type phases. In particular, we express the strength of Dirac-type CP violation in terms of these Majorana-type phases by writing the area of the unitarity triangles in terms of these phases. We also study how these six Majorana ph...
متن کامل9 v 1 1 6 D ec 1 99 8 Does Weak CP Phase Originate from a Certain Geometry ?
We further investigate the probability that, weak CP phase originates in a certain geometry. We find that our postulation on weak CP Phase gives strict constraints on angle γ in unitarity triangle DB and the element Vtd in Cabibbo-Kobayashi-Maskawa (CKM) matrix. The predicted |Vtd| is about 0.0086 and γ about 75.3 0 with the very narrow window respectively. These two parameters can be used to t...
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 2002