Cabibbo-Kobayashi-Maskawa matrix

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Flavour in particle physics
Flavour quantum numbers: Lepton number: L Baryon number: B Strangeness: S Charm: C Bottomness: B' Topness: T Isospin: I_z or I Weak isospin: T_z Electric charge: Q Combinations: Hypercharge: Y Y=2(Q-I_z) Y=B+S+C+B'+T Weak hypercharge: Y_W Y_W=2(Q-T_z) Y_W=B−L Related topics: CPT symmetry CKM matrix CP symmetry Chirality

In the standard model of particle physics the Cabibbo-Kobayashi-Maskawa matrix (CKM matrix, quark mixing matrix, sometimes earlier called KM matrix) is a unitary matrix which contains information on the strength of flavour-changing weak decays. Technically, it specifies the mismatch of quantum states of quarks when they propagate freely and when they take part in the weak interactions. It is important in the understanding of CP violations. A precise mathematical definition of this matrix is given in the article on the formulation of the standard model. This matrix was introduced for three generations of quarks by Makoto Kobayashi and Toshihide Maskawa, adding one generation to the matrix previously introduced by Nicola Cabibbo.

1 The matrix
2 Counting
3 Observations and predictions
4 Weak universality
5 The unitarity triangles
6 See also
7 References
8 External links

[edit] The matrix

$\begin{bmatrix} V_{ud} & V_{us} & V_{ub} \\ V_{cd} & V_{cs} & V_{cb} \\ V_{td} & V_{ts} & V_{tb} \end{bmatrix} \begin{bmatrix} \left| d \right \rangle \\ \left| s \right \rangle \\ \left| b \right \rangle \end{bmatrix} = \begin{bmatrix} \left| d' \right \rangle \\ \left| s' \right \rangle \\ \left| b' \right \rangle \end{bmatrix}$

On the left is the CKM Matrix along with a vector of strong force eigenstates of the quarks, and on the right is the weak force eigenstates of the quarks. The CKM matrix describes the probability of a transition from one quark q to another quark q' . This transition is proportional to $\left| V_{qq'} \right| ^2$ .

Experimentally, the magnitudes of the values in the matrix have been found to be roughly:

$\begin{bmatrix} 0.9753 & 0.221 & 0.003 \\ 0.221 & 0.9747 & 0.040 \\ 0.009 & 0.039 & 0.9991 \end{bmatrix}$

[edit] Counting

To proceed further, it is necessary to count the number of parameters in this matrix, V which appear in experiments, and therefore are physically important. If there are N generations of quarks (2N flavours) then

An N×N complex matrix contains 2N² real numbers.
The constraint of unitarity is ∑_k V_ikV^*_jk = δ_ij. Therefore, for the diagonal terms (i=j) there are N constraints, and for the remaining terms, N(N−1). The number of independent real numbers in an unitary matrix is therefore N².
One phase can be absorbed into each quark field. An overall common phase is unobservable. Hence there are 2N−1 less independent numbers, giving the total number of free variables to be (N−1)².
Of these, N(N−1)/2 are rotation angles called quark mixing angles.
The remaining (N−1)(N−2)/2 are complex phases, which cause CP violation.

For the case N=2, there is only one parameter which is a mixing angle between two generations of quarks. Historically, this was the first version of CKM matrix when only two generations were known. It is called the Cabibbo angle after its inventor Nicola Cabibbo.

For the Standard Model case N=3, there are three mixing angles and one CP-violating complex phase.

[edit] Observations and predictions

Cabibbo's idea originated from a need to explain two observed phenomena:

the transitions u↔d and e↔ν_e, μ↔ν_μ had similar amplitudes.
the transitions with change in strangeness ΔS=1 had amplitudes equal to 1/4 of those with ΔS=0.

Cabibbo's solution consisted of postulating weak universality to resolve issue 1, along with a mixing angle θ_c, now called the Cabibbo angle, between the d and s quarks to resolve issue 2.

For two generations of quarks, there are no CP violating phases, as shown by the counting of the previous section. Since CP violations were seen in neutral kaon decays already in 1964, the emergence of the standard model soon after was a clear signal of the existence of a third generation of quarks, as pointed out in 1973 by Kobayashi and Maskawa. The discovery of the bottom quark at Fermilab (by Leon Lederman's group) in 1976 therefore immediately started off the search for the missing third-generation quark, the top quark.

[edit] Weak universality

The constraints of unitarity of the CKM-matrix on the diagonal terms can be written as

∑	\| V_ij \| ² = 1
j

for all generations i. This implies that the sum of all couplings of any of the up-type quarks to all the down-type quarks is the same for all generations. This relation is called weak universality after Nicola Cabibbo, who first pointed it out in 1967. Theoretically it is a consequence of the fact that all SU(2) doublets couple with the same strength to the vector bosons of weak interactions. It has been subjected to continuing experimental tests.

[edit] The unitarity triangles

The remaining constraints of unitarity of the CKM-matrix can be written in the form

$\sum_k V_{ik}V^*_{jk} = 0$

For any fixed i and j, this is a constraint on three complex numbers, one for each k, which says that these numbers form the vertices of a triangle in the complex plane. There are six choices of i and j, and hence six such triangles, each of which is called an unitary triangle. Their shapes can be very different, but they all have the same area, which can be related to the CP violating phase. The area vanishes for the specific parameters in the standard model for which there would be no CP violation. The orientation of the triangles depend on the phases of the quark fields.

Since the three sides of the triangles are open to direct experiment, as are the three angles, a class of tests of the standard model is to check that the triangle closes. This is the purpose of a modern series of experiments under way at the Japanese BELLE and the Californian BaBar experiments.

[edit] See also

Formulation of the standard model and CP violations.
Quantum chromodynamics, flavour and strong CP problem.
MNS matrix, the equivalent mixing matrix for neutrinos.

[edit] References

Griffiths, David J. (1987). Introduction to Elementary Particles. Wiley, John & Sons, Inc. ISBN 0-471-60386-4.
Povh, Bogdan et al., (1995). Particles and Nuclei: An Introduction to the Physical Concepts. New York: Springer. ISBN 3-540-20168-8