RECENT RESULTS FROM THE TEVATRON ON CKM MATRIX ELEMENTS FROM Bs OSCILLATIONS AND SINGLE TOP PRODUCTION, AND STUDIES OF CP VIOLATION IN Bs DECAYS

2009 ◽  
Author(s):  
J.P. Fernández
Keyword(s):  
Cp Violation ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
Single Top ◽  
Ckm Matrix Elements

scholarly journals Measurement of CKM matrix elements in single top quark t-channel production in proton-proton collisions at s=13 TeV

2020 ◽  
Vol 808 ◽  
pp. 135609
Author(s):  
A.M. Sirunyan ◽  
A. Tumasyan ◽  
W. Adam ◽  
F. Ambrogi ◽  
T. Bergauer ◽  
...  
Keyword(s):  
Top Quark ◽  
Matrix Elements ◽  
Proton Proton ◽  
Ckm Matrix ◽  
Proton Collisions ◽  
Single Top ◽  
Ckm Matrix Elements ◽  
Proton Proton Collisions

scholarly journals FRITZSCH-LIKE QUARK MASS MATRICES WITH DECOUPLED u QUARK

1994 ◽  
Vol 09 (26) ◽  
pp. 2461-2467 ◽  
Author(s):  
P.S. GILL ◽  
MANMOHAN GUPTA
Keyword(s):  
Cp Violation ◽  
Quark Mass ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
Mass Matrices ◽  
Ckm Matrix Elements ◽  
Invariant Parameter

Fritzsch-like Hermitian quark mass matrices with decoupled u quark as well as nonzero 22-elements, both in ‘U’ and ‘D’ sectors, have been considered to reconcile the data regarding [Formula: see text] and CKM matrix elements. Exploiting the idea of maximality of CP-violation, we find two interesting relations between CKM matrix elements, viz. |Vtd|≅ |Vus||Vcb|, |Vub|≅ ½(ms/ mb)|Vus|. Apart from obtaining 0.05≤|Vub/Vcb|≤0.12 and [Formula: see text], we find CP-violating rephasing invariant parameter |J|≅(3–5)×10−5. The predicted |Vtd| value implies almost maximal mixing in [Formula: see text] system.

CKM MATRIX ELEMENTS AND MAXIMALITY OF CP-VIOLATION

1998 ◽  
Vol 13 (30) ◽  
pp. 2445-2452 ◽  
Author(s):  
P. S. GILL ◽  
MANMOHAN GUPTA
Keyword(s):  
Cp Violation ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
Ckm Matrix Elements

Maximality of CP-violation is defined by maximizing the Jarlskog rephasing invariant |J| which is twice the area of any of the six unitarity triangles. When the area of two of the unitarity triangles is maximized w.r.t.|Vtd|, we obtain |Vtd|=(8.5-10.2)×10-3 and CP violating phase δ=60°-168°. Two well-known triangles yield J expt =(2.2-3.7)×10-5 which leads to δ = 33°-146° and |Vtd|=(5.6-13.1)×10-3. When the constraints due to "maximality" and J expt are considered simultaneously, we obtain |Vtd|=(8.5-10.2)×10-3 and δ=60°-136°.

scholarly journals Progress on semi-leptonic B(s) decays

2014 ◽  
Vol 29 (20) ◽  
pp. 1430019 ◽  
Author(s):  
Giulia Ricciardi
Keyword(s):  
Rare Decays ◽  
Current Status ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
The Absolute ◽  
Ckm Matrix Elements

We report on the current status of semi-leptonic B(s) decays, including rare decays, and the extraction of the absolute values of the CKM matrix elements |Vcb| and |Vub|.

scholarly journals THE DUALIZED STANDARD MODEL AND ITS APPLICATIONS — AN INTERIM REPORT

1999 ◽  
Vol 14 (14) ◽  
pp. 2173-2203 ◽  
Author(s):  
HONG-MO CHAN ◽  
SHEUNG TSUN TSOU
Keyword(s):  
Standard Model ◽  
High Energy ◽  
Fermion Mass ◽  
Mass Hierarchy ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
High Energy Cosmic Rays ◽  
Perturbative Method ◽  
Ckm Matrix Elements ◽  
Physical Consequences

Based on a non-Abelian generalization of electric–magnetic duality, the Dualized Standard Model (DSM) suggests a natural explanation for exactly three generations of fermions as the "dual colour" [Formula: see text] symmetry broken in a particular manner. The resulting scheme then offers on the one hand a fermion mass hierarchy and a perturbative method for calculating the mass and mixing parameters of the Standard Model fermions, and on the other hand testable predictions for new phenomena ranging from rare meson decays to ultra-high energy cosmic rays. Calculations to one-loop order gives, at the cost of adjusting only three real parameters, values for the following quantities all (except one) in very good agreement with experiment: the quark CKM matrix elements ‖Vrs‖, the lepton CKM matrix elements ‖Urs‖, and the second generation masses mc, ms, mμ. This means, in particular, that it gives near maximal mixing Uμ3 between νμ and ντ as observed by SuperKamiokande, Kamiokande and Soudan, while keeping small the corresponding quark angles Vcb, Vts. In addition, the scheme gives (i) rough order-of-magnitude estimates for the masses of the lowest generation, (ii) predictions for low energy FCNC effects such as KL→ eμ, and (iii) a possible explanation for the long-standing puzzle of air showers beyond the GZK cut-off. All these together, however, still represent but a portion of the possible physical consequences derivable from the DSM scheme, the majority of which are yet to be explored.

Chapter 22 Leptonic, Semileptonic D(DS) Decays and CKM Matrix Elements

2009 ◽  
Vol 24 (supp01) ◽  
pp. 521-567
Author(s):  
Ya-Dong Yang ◽  
Hai-Bo Li ◽  
Jia-Heng Zou ◽  
Jiang-Chuan Chen ◽  
Jian Liu ◽  
...  
Keyword(s):  
Semileptonic Decays ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
Leptonic Decays ◽  
Ckm Matrix Elements

The following sections are included: Leptonic Decays Semileptonic Decays Impact on CKM Measurements

scholarly journals A REVIEW OF THE MAGNITUDES OF THE CKM MATRIX ELEMENTS

2008 ◽  
Vol 23 (31) ◽  
pp. 4945-4958 ◽  
Author(s):  
FRANCESCA DI LODOVICO
Keyword(s):  
Standard Model ◽  
Current Status ◽  
Matrix Elements ◽  
Ckm Matrix ◽  
The Standard Model ◽  
The Matrix ◽  
The Absolute ◽  
Ckm Matrix Elements

Flavour mixing is described within the Standard Model by the Cabibbo–Kobayashi–Maskawa (CKM) matrix elements. With the increasingly higher statistics collected by many experiments, the matrix elements are measured with improved precision, allowing for more stringent tests of the Standard Model. In this paper, a review of the current status of the absolute values of the CKM matrix elements is presented, with particular attention to the latest measurements.

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