Particle Physics Booklet - Particle Data Group - Lawrence Berkeley ...

11. The CKM quark-mixing matrix 181
11. THE CKM QUARK-MIXING MATRIX
Revised February 2010 by A. Ceccucci (CERN), Z. Ligeti (LBNL), and
Y. Sakai (KEK).
11.1. Introduction
The masses and mixings of quarks have a common origin in the
Standard Model (SM). They arise from the Yukawa interactions of the
quarks with the Higgs condensate. When the Higgs field acquires a vacuum
expectation value, quark mass terms are generated. The physical states are
obtained by diagonalizing the up and down quark mass matrices by four
unitary matrices, V u,d
L,R . As a result, the charged current W ± interactions
couple to the physical up and down-type quarks with couplings given by
VCKM ≡ V u d†
L VL =
⎛
⎝ V ⎞
ud Vus Vub Vcd Vcs V ⎠
cb . (11.2)
Vtd Vts Vtb This Cabibbo-Kobayashi-Maskawa (CKM) matrix [1,2] is a 3 × 3
unitary matrix. It can be parameterized by three mixing angles and a
CP-violating phase,
⎛
⎞
V = ⎝
c 12 c 13 s 12 c 13 s 13 e −iδ
−s 12 c 23 −c 12 s 23 s 13 e iδ c 12 c 23 −s 12 s 23 s 13 e iδ s 23 c 13
s 12 s 23 −c 12 c 23 s 13 e iδ −c 12 s 23 −s 12 c 23 s 13 e iδ c 23 c 13
⎠ , (11.3)
where sij =sinθij, cij =cosθij, andδis the phase responsible for all
CP-violating phenomena in flavor changing processes in the SM. The
angles θij can be chosen to lie in the first quadrant.
It is known experimentally that s13 ≪ s23 ≪ s12 ≪ 1, and it is
convenient to exhibit this hierarchy using the Wolfenstein parameterization.
We define [4–6]
|Vus|
s12 = λ = �
|Vud| 2 + |Vus| 2 , s23 = Aλ 2 � �
�
= λ �
Vcb �
�
�Vus
� ,
s13e iδ = V ∗ ub = Aλ3 (ρ + iη) = Aλ3 (¯ρ + i¯η) √ 1 − A 2 λ 4
√ 1 − λ 2 [1 − A 2 λ 4 (¯ρ + i¯η)] . (11.4)
These ensure that ¯ρ + i¯η = −(VudV ∗ ub )/(VcdV ∗
cb ) is phase-convention
independent and the CKM matrix written in terms of λ, A, ¯ρ and ¯η is
unitary to all orders in λ. To O(λ4 ),
⎛
V = ⎝ 1 − λ2 /2 λ Aλ3 (ρ − iη)
−λ 1 − λ2 /2 Aλ2 Aλ3 (1 − ρ − iη) −Aλ2 ⎞
⎠ + O(λ
1
4 ) . (11.5)
Unitarity implies �
i VijV
∗
ik = δjk and �
j VijV
∗
kj = δik. Thesix
vanishing combinations can be represented as triangles in a complex plane.
The most commonly used unitarity triangle arises from
Vud V ∗ ub + Vcd V ∗
cb + Vtd V ∗
tb =0, (11.6)
by dividing each side by VcdV ∗
cb (see Fig. 1). The vertices are exactly (0, 0),
(1, 0) and, due to the definition in Eq. (11.4), (¯ρ, ¯η). An important goal of
flavor physics is to overconstrain the CKM elements, many of which can
be displayed and compared in the ¯ρ, ¯η plane.