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In the Standard Model of particle physics, the Cabibbo–Kobayashi–Maskawa matrix, CKM matrix, quark mixing matrix, or KM matrix is a unitary matrix which contains information on the strength of the flavour-changing weak interaction. 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 violation. 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. This matrix is also an extension of the GIM mechanism, which only includes two of the three current families of quarks.

The matrix
Predecessor: Cabibbo matrix
The Cabibbo angle represents the rotation of the mass eigenstate vector space formed by the mass eigenstates \( \scriptstyle {|d\rangle ,\ |s\rangle } \) into the weak eigenstate vector space formed by the weak eigenstates \( \scriptstyle {|d^{\prime }\rangle ,\ |s^{\prime }\rangle } \). θC = 13.02°.

In 1963, Nicola Cabibbo introduced the Cabibbo angle (θc) to preserve the universality of the weak interaction.[1] Cabibbo was inspired by previous work by Murray Gell-Mann and Maurice Lévy,[2] on the effectively rotated nonstrange and strange vector and axial weak currents, which he references.[3]

In light of current knowledge (quarks were not yet theorized), the Cabibbo angle is related to the relative probability that down and strange quarks decay into up quarks (|Vud|2 and |Vus|2 respectively). In particle physics parlance, the object that couples to the up quark via charged-current weak interaction is a superposition of down-type quarks, here denoted by d′.[4] Mathematically this is:

\( d^{\prime }=V_{ud}d+V_{us}s, \)

or using the Cabibbo angle:

\( d^{\prime }=\cos \theta _{\mathrm {c} }d+\sin \theta _{\mathrm {c} }s. \)

Using the currently accepted values for |Vud| and |Vus| (see below), the Cabibbo angle can be calculated using

\( {\displaystyle \tan \theta _{\mathrm {c} }={\frac {|V_{us}|}{|V_{ud}|}} ={\frac {0.22534}{0.97427}}\Rightarrow \theta _{\mathrm {c} }=~13.02^{\circ }.} \)

When the charm quark was discovered in 1974, it was noticed that the down and strange quark could decay into either the up or charm quark, leading to two sets of equations:

\( d^{\prime }=V_{ud}d+V_{us}s; \)
\( s^{\prime }=V_{cd}d+V_{cs}s, \)

or using the Cabibbo angle:

\( d^{\prime }=\cos {\theta _{\mathrm {c} }}d+\sin {\theta _{\mathrm {c} }}s;

\(s^{\prime }=-\sin {\theta _{\mathrm {c} }}d+\cos {\theta _{\mathrm {c} }}s.

This can also be written in matrix notation as:

\( {\begin{bmatrix}d^{\prime }\\s^{\prime }\end{bmatrix}}={\begin{bmatrix}V_{ud}&V_{us}\\V_{cd}&V_{cs}\\\end{bmatrix}} {\begin{bmatrix}d\\s\end{bmatrix}}, \)

or using the Cabibbo angle

\( {\begin{bmatrix}d^{\prime }\\s^{\prime }\end{bmatrix}}={\begin{bmatrix}\cos {\theta _{\mathrm {c} }} &\sin {\theta _{\mathrm {c} }}\\-\sin {\theta _{\mathrm {c} }} &\cos {\theta _{\mathrm {c} }}\\\end{bmatrix}}{\begin{bmatrix}d\\s\end{bmatrix}}, \)

where the various |Vij|2 represent the probability that the quark of j flavor decays into a quark of i flavor. This 2 × 2 rotation matrix is called the Cabibbo matrix.
A pictorial representation of the six quarks' decay modes, with mass increasing from left to right.
CKM matrix

In 1973, observing that CP-violation could not be explained in a four-quark model, Kobayashi and Maskawa generalized the Cabibbo matrix into the Cabibbo–Kobayashi–Maskawa matrix (or CKM matrix) to keep track of the weak decays of three generations of quarks:[5]

\( {\begin{bmatrix}d^{\prime }\\s^{\prime }\\b^{\prime }\end{bmatrix}}={\begin{bmatrix}V_{ud}&V_{us}&V_{ub}\\V_{cd}&V_{cs}&V_{cb}\\V_{td} &V_{ts}&V_{tb}\end{bmatrix}}{\begin{bmatrix}d\\s\\b\end{bmatrix}}. \)

On the left is the weak interaction doublet partners of down-type quarks, and on the right is the CKM matrix along with a vector of mass eigenstates of down-type quarks. The CKM matrix describes the probability of a transition from one quark i to another quark j. These transitions are proportional to |Vij|2.

As of 2010, the best determination of the magnitudes of the CKM matrix elements was:[6]

\( {\begin{bmatrix}|V_{ud}|&|V_{us}|&|V_{ub}|\\|V_{cd}|&|V_{cs}|&|V_{cb}|\\|V_{td}| &|V_{ts}|&|V_{tb}|\end{bmatrix}} ={\begin{bmatrix}0.97427\pm 0.00015&0.22534\pm 0.00065&0.00351_{-0.00014}^{+0.00015}\\0.22520\pm 0.00065 &0.97344\pm 0.00016&0.0412_{-0.0005}^{+0.0011}\\0.00867_{-0.00031}^{+0.00029}&0.0404_{-0.0005}^{+0.0011}&0.999146_{-0.000046}^{+0.000021}\end{bmatrix}}. \)

The choice of usage of down-type quarks in the definition is a convention, and does not represent a physically preferred asymmetry between up-type and down-type quarks. Other conventions are equally valid, such as defining the matrix in terms of weak interaction partners of mass eigenstates of up-type quarks, u′, c′ and t′, in terms of u, c, and t. Since the CKM matrix is unitary, its inverse is the same as its conjugate transpose.
General case construction

To generalize the matrix, count the number of physically important parameters in this matrix, V which appear in experiments. If there are N generations of quarks (2N flavours) then

An N × N unitary matrix (that is, a matrix V such that VV† = I, where V† is the conjugate transpose of V and I is the identity matrix) requires N2 real parameters to be specified.
2N − 1 of these parameters are not physically significant, because one phase can be absorbed into each quark field (both of the mass eigenstates, and of the weak eigenstates), but the matrix is independent of a common phase. Hence, the total number of free variables independent of the choice of the phases of basis vectors is N2 − (2N − 1) = (N − 1)2.
Of these, 1/2N(N − 1) are rotation angles called quark mixing angles.
The remaining 1/2(N − 1)(N − 2) are complex phases, which cause CP violation.

N = 2

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.
N = 3

For the Standard Model case (N = 3), there are three mixing angles and one CP-violating complex phase.[7]
Observations and predictions

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

the transitions u ↔ d, e ↔ νe, and μ ↔ νμ 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 the first issue, along with a mixing angle θc, now called the Cabibbo angle, between the d and s quarks to resolve the second.

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.

Note, however, that the specific values of the angles are not a prediction of the standard model: they are open, unfixed parameters. At this time, there is no generally accepted theory that explains why the measured values are what they are.
Weak universality

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

\( \sum _{k}|V_{ik}|^{2}=\sum _{i}|V_{ik}|^{2}=1 \)

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 and was first pointed out by Nicola Cabibbo 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.
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 and different i and j, this is a constraint on three complex numbers, one for each k, which says that these numbers form the sides of a triangle in the complex plane. There are six choices of i and j (three independent), and hence six such triangles, each of which is called a 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.

A popular quantity amounting to twice the area of the unitarity triangle is the Jarlskog invariant,

\( {\displaystyle J=c_{12}c_{13}^{2}c_{23}s_{12}s_{13}s_{23}\sin \delta \approx 3\cdot 10^{-5}.} \)

For Greek indices denoting up quarks and Latin ones down quarks, the 4-tensor\( {\displaystyle (\alpha ,\beta ;i,j)\equiv \operatorname {Im} (V_{\alpha i}V_{\beta j}V_{\alpha j}^{*}V_{\beta i}^{*})} \) is doubly antisymmetric,

\( {\displaystyle (\beta ,\alpha ;i,j)=-(\alpha ,\beta ;i,j)=(\alpha ,\beta ;j,i).} \)

Up to antisymmetry, it only has 9 = 3 × 3 non-vanishing components, which, remarkably, from the unitarity of V, can be shown to be all identical in magnitude, that is,

\( {\displaystyle (\alpha ,\beta ;i,j)=J~{\begin{bmatrix}0&1&-1\\-1&0&1\\1&-1&0\end{bmatrix}}_{\alpha \beta }\otimes {\begin{bmatrix}0&1&-1\\-1&0&1\\1&-1&0\end{bmatrix}}_{ij},} \)

so that

\( {\displaystyle J=(u,c;s,b)=(u,c;d,s)=(u,c;b,d)=(c,t;s,b)=(c,t;d,s)=(c,t;b,d)=(t,u;s,b)=(t,u;b,d)=(t,u;d,s).} \)

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 American BaBar experiments, as well as at LHCb in CERN, Switzerland.

Four independent parameters are required to fully define the CKM matrix. Many parameterizations have been proposed, and three of the most common ones are shown below.
KM parameters

The original parameterization of Kobayashi and Maskawa used three angles ( θ1, θ2, θ3 ) and a CP-violating phase angle ( δ ).[5] θ1 is the Cabibbo angle. Cosines and sines of the angles θk are denoted ck and sk, for k = 1, 2, 3 respectively.

\( {\begin{bmatrix}c_{1}&-s_{1}c_{3}&-s_{1}s_{3}\\s_{1}c_{2} &c_{1}c_{2}c_{3}-s_{2}s_{3}e^{i\delta } &c_{1}c_{2}s_{3}+s_{2}c_{3}e^{i\delta }\\s_{1}s_{2}&c_{1}s_{2}c_{3}+c_{2}s_{3}e^{i\delta } &c_{1}s_{2}s_{3}-c_{2}c_{3}e^{i\delta }\end{bmatrix}}. \)

"Standard" parameters

A "standard" parameterization of the CKM matrix uses three Euler angles ( θ12, θ23, θ13 ) and one CP-violating phase ( δ13 ).[8] θ12 is the Cabibbo angle. Couplings between quark generations j and k vanish if θjk = 0 . Cosines and sines of the angles are denoted cjk and sjk, respectively.

\( {\begin{aligned}&{\begin{bmatrix}1&0&0\\0&c_{23}&s_{23}\\0&-s_{23} &c_{23}\end{bmatrix}}{\begin{bmatrix}c_{13} &0&s_{13}e^{-i\delta _{13}}\\0&1&0\\-s_{13}e^{i\delta _{13}}&0&c_{13}\end{bmatrix}}{\begin{bmatrix}c_{12} &s_{12}&0\\-s_{12}&c_{12}&0\\0&0&1\end{bmatrix}}\\&={\begin{bmatrix}c_{12}c_{13} &s_{12}c_{13} &s_{13}e^{-i\delta _{13}}\\-s_{12}c_{23}-c_{12}s_{23}s_{13}e^{i\delta _{13}}&c_{12}c_{23}-s_{12}s_{23}s_{13}e^{i\delta _{13}} &s_{23}c_{13}\\s_{12}s_{23}-c_{12}c_{23}s_{13}e^{i\delta _{13}}&-c_{12}s_{23}-s_{12}c_{23}s_{13}e^{i\delta _{13}}&c_{23}c_{13}\end{bmatrix}}.\end{aligned}} \)

The currently best known values for the standard parameters are:[9]

θ12 = 13.04±0.05°, θ13 = 0.201±0.011°, θ23 = 2.38±0.06°, and δ13 = 1.20±0.08 radians.

Wolfenstein parameters

A third parameterization of the CKM matrix was introduced by Lincoln Wolfenstein with the four parameters λ, A, ρ, and η.[10] The four Wolfenstein parameters have the property that all are of order 1 and are related to the "standard" parameterization:

λ = s12
A λ2 = s23
A λ3 ( ρ − iη ) = s13 e−iδ

The Wolfenstein parameterization of the CKM matrix, is an approximation of the standard parameterization. To order λ3, it is:

\( {\displaystyle {\begin{bmatrix}1-{\tfrac {1}{2}}\lambda ^{2}&\lambda &A\lambda ^{3}(\rho -i\eta )\\-\lambda &1-{\tfrac {1}{2}}\lambda ^{2}&A\lambda ^{2}\\A\lambda ^{3}(1-\rho -i\eta )&-A\lambda ^{2}&1\end{bmatrix}}+O(\lambda ^{4}).} \)

The CP violation can be determined by measuring ρ − iη.

Using the values of the previous section for the CKM matrix, the best determination of the Wolfenstein parameters is:[11]

λ = 0.2257+0.0009
−0.0010, A = 0.814+0.021
−0.022, ρ = 0.135+0.031
−0.016, and η = 0.349+0.015
−0.017 .

Nobel Prize

In 2008, Kobayashi and Maskawa shared one half of the Nobel Prize in Physics "for the discovery of the origin of the broken symmetry which predicts the existence of at least three families of quarks in nature".[12] Some physicists were reported to harbor bitter feelings about the fact that the Nobel Prize committee failed to reward the work of Cabibbo, whose prior work was closely related to that of Kobayashi and Maskawa.[13] Asked for a reaction on the prize, Cabibbo preferred to give no comment.[14]
See also

Formulation of the Standard Model and CP violations
Quantum chromodynamics, flavour and strong CP problem
Weinberg angle, a similar angle for Z and photon mixing
Pontecorvo–Maki–Nakagawa–Sakata matrix, the equivalent mixing matrix for neutrinos
Koide formula


Cabibbo, N. (1963). "Unitary Symmetry and Leptonic Decays". Physical Review Letters. 10 (12): 531–533. Bibcode:1963PhRvL..10..531C. doi:10.1103/PhysRevLett.10.531.
Gell-Mann, M.; Lévy, M. (1960). "The Axial Vector Current in Beta Decay". Il Nuovo Cimento. 16 (4): 705–726. Bibcode:1960NCim...16..705G. doi:10.1007/BF02859738. S2CID 122945049.
Maiani, L. (2009). "Sul Premio Nobel Per La Fisica 2008" (PDF). Il Nuovo Saggiatore. 25 (1–2): 78. Archived from the original (PDF) on 22 July 2011. Retrieved 30 November 2010.
Hughes, I.S. (1991). "Chapter 11.1 – Cabibbo Mixing". Elementary Particles (3rd ed.). Cambridge University Press. pp. 242–243. ISBN 978-0-521-40402-0.
Kobayashi, M.; Maskawa, T. (1973). "CP-Violation in the Renormalizable Theory of Weak Interaction". Progress of Theoretical Physics. 49 (2): 652–657. Bibcode:1973PThPh..49..652K. doi:10.1143/PTP.49.652.
Beringer, J.; Arguin, J.-F.; Barnett, R.M.; Copic, K.; Dahl, O.; Groom, D.E.; et al. (2012). "Review of Particle Physics: The CKM Quark-Mixing Matrix" (PDF). Physical Review D. 80 (1): 1–1526 [162]. Bibcode:2012PhRvD..86a0001B. doi:10.1103/PhysRevD.86.010001.
Baez, J.C. (4 April 2011). "Neutrinos and the Mysterious Pontecorvo-Maki-Nakagawa-Sakata Matrix". Retrieved 13 February 2016. "In fact, the Pontecorvo–Maki–Nakagawa–Sakata matrix actually affects the behavior of all leptons, not just neutrinos. Furthermore, a similar trick works for quarks – but then the matrix U is called the Cabibbo–Kobayashi–Maskawa matrix."
Chau, L.L.; Keung, W.-Y. (1984). "Comments on the Parametrization of the Kobayashi-Maskawa Matrix". Physical Review Letters. 53 (19): 1802–1805. Bibcode:1984PhRvL..53.1802C. doi:10.1103/PhysRevLett.53.1802.
Values obtained from values of Wolfenstein parameters in the 2008 Review of Particle Physics.
Wolfenstein, L. (1983). "Parametrization of the Kobayashi-Maskawa Matrix". Physical Review Letters. 51 (21): 1945–1947. Bibcode:1983PhRvL..51.1945W. doi:10.1103/PhysRevLett.51.1945.
Amsler, C.; Doser, M.; Antonelli, M.; Asner, D.M.; Babu, K.S.; Baer, H.; et al. (Particle Data Group) (2008). "Review of Particles Physics: The CKM Quark-Mixing Matrix" (PDF). Physics Letters B. 667 (1): 1–1340. Bibcode:2008PhLB..667....1A. doi:10.1016/j.physletb.2008.07.018.
"The Nobel Prize in Physics 2008" (Press release). The Nobel Foundation. 7 October 2008. Retrieved 24 November 2009.
Jamieson, V. (7 October 2008). "Physics Nobel Snubs key Researcher". New Scientist. Retrieved 24 November 2009.

"Nobel, l'amarezza dei fisici italiani". Corriere della Sera (in Italian). 7 October 2008. Retrieved 24 November 2009.

Further reading and external links

D.J Griffiths (2008). Introduction to Elementary Particles (2nd ed.). John Wiley & Sons. ISBN 978-3-527-40601-2.

B. Povh; et al. (1995). Particles and Nuclei: An Introduction to the Physical Concepts. Springer. ISBN 978-3-540-20168-7.

I.I. Bigi, A.I. Sanda (2000). CP violation. Cambridge University Press. ISBN 978-0-521-44349-4.

"Particle Data Group: The CKM quark-mixing matrix" (PDF).

"Particle Data Group: CP violation in meson decays" (PDF).

"The Babar experiment". at SLAC, California, and "the BELLE experiment". at KEK, Japan.


Matrix classes
Explicitly constrained entries

(0,1) Alternant Anti-diagonal Anti-Hermitian Anti-symmetric Arrowhead Band Bidiagonal Binary Bisymmetric Block-diagonal Block Block tridiagonal Boolean Cauchy Centrosymmetric Conference Complex Hadamard Copositive Diagonally dominant Diagonal Discrete Fourier Transform Elementary Equivalent Frobenius Generalized permutation Hadamard Hankel Hermitian Hessenberg Hollow Integer Logical Markov Metzler Monomial Moore Nonnegative Partitioned Parisi Pentadiagonal Permutation Persymmetric Polynomial Positive Quaternionic Sign Signature Skew-Hermitian Skew-symmetric Skyline Sparse Sylvester Symmetric Toeplitz Triangular Tridiagonal Unitary Vandermonde Walsh Z


Exchange Hilbert Identity Lehmer Of ones Pascal Pauli Redheffer Shift Zero

Conditions on eigenvalues or eigenvectors

Companion Convergent Defective Diagonalizable Hurwitz Positive-definite Stability Stieltjes

Satisfying conditions on products or inverses

Congruent Idempotent or Projection Invertible Involutory Nilpotent Normal Orthogonal Orthonormal Singular Unimodular Unipotent Totally unimodular Weighing

With specific applications

Adjugate Alternating sign Augmented Bézout Carleman Cartan Circulant Cofactor Commutation Confusion Coxeter Derogatory Distance Duplication Elimination Euclidean distance Fundamental (linear differential equation) Generator Gramian Hessian Householder Jacobian Moment Payoff Pick Random Rotation Seifert Shear Similarity Symplectic Totally positive Transformation Wedderburn X–Y–Z

Used in statistics

Bernoulli Centering Correlation Covariance Design Dispersion Doubly stochastic Fisher information Hat Precision Stochastic Transition

Used in graph theory

Adjacency Biadjacency Degree Edmonds Incidence Laplacian Seidel adjacency Skew-adjacency Tutte

Used in science and engineering

Cabibbo–Kobayashi–Maskawa Density Fundamental (computer vision) Fuzzy associative Gamma Gell-Mann Hamiltonian Irregular Overlap S State transition Substitution Z (chemistry)

Related terms

Jordan canonical form Linear independence Matrix exponential Matrix representation of conic sections Perfect matrix Pseudoinverse Quaternionic matrix Row echelon form Wronskian

List of matrices Category:Matrices


Standard Model

Particle physics
Fermions Gauge boson Higgs boson Quantum field theory Gauge theory Strong interaction
Color charge Quantum chromodynamics Quark model Electroweak interaction
Weak interaction Quantum electrodynamics Fermi's interaction Weak hypercharge Weak isospin


CKM matrix Spontaneous symmetry breaking Higgs mechanism Mathematical formulation of the Standard Model

Beyond the
Standard Model

Hierarchy problem Dark matter Cosmological constant problem Strong CP problem Neutrino oscillation


Technicolor Kaluza–Klein theory Grand Unified Theory Theory of everything


MSSM Superstring theory Supergravity

Quantum gravity

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