Английская Википедия:Cabibbo–Kobayashi–Maskawa matrix

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 – the Cabibbo matrix

Файл:Cabibbo angle.svg

\, s' \rangle ~.</math> Шаблон:Nowrap

In 1963, Nicola Cabibbo introduced the Cabibbo angle (Шаблон:Mvar Шаблон:Sub) 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 concepts (quarks had not yet been proposed), the Cabibbo angle is related to the relative probability that down and strange quarks decay into up quarks ( |Шаблон:Mvar Шаблон:Sub|Шаблон:Sup and |Шаблон:Mvar Шаблон:Sub|Шаблон:Sup , respectively). In particle physics jargon, the object that couples to the up quark via charged-current weak interaction is a superposition of down-type quarks, here denoted by Шаблон:Mvar.^[4] Mathematically this is:

<math> d' = V_\mathrm{ud} \; d ~~ + ~~ V_\mathrm{us} \; s ~,</math>

or using the Cabibbo angle:

<math> d' = \cos \theta_\mathrm{c} \; d ~~ + ~~ \sin \theta_\mathrm{c} \; s ~.</math>

Using the currently accepted values for |Шаблон:Mvar Шаблон:Sub| and |Шаблон:Mvar Шаблон:Sub| (see below), the Cabibbo angle can be calculated using

<math> \tan\theta_\mathrm{c} = \frac{\, |V_\mathrm{us}| \,}{|V_\mathrm{ud}|} = \frac{0.22534}{0.97427} \quad \Rightarrow \quad \theta_\mathrm{c}= ~13.02^\circ ~.</math>

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:

<math> d' = V_\mathrm{ud} \; d ~~ + ~~ V_\mathrm{us} \; s ~,</math>

<math> s' = V_\mathrm{cd} \; d ~~ + ~~ V_\mathrm{cs} \; s ~;</math>

or using the Cabibbo angle:

<math> d' = EducationBot (обсуждение) \cos{\theta_\mathrm{c}} \; d ~~+~~ \sin{\theta_\mathrm{c}} \; s ~,</math>

<math> s' = - \sin{\theta_\mathrm{c}} \; d ~~+~~ \cos{\theta_\mathrm{c}} \; s ~.</math>

This can also be written in matrix notation as:

<math>

\begin{bmatrix} d' \\ s' \end{bmatrix} = \begin{bmatrix} V_\mathrm{ud} & V_\mathrm{us} \\ V_{cd} & V_{cs} \\ \end{bmatrix} \begin{bmatrix} d \\ s \end{bmatrix} ~, </math>

or using the Cabibbo angle

<math>

\begin{bmatrix} d' \\ s' \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}~, </math>

where the various |Шаблон:Mvar|Шаблон:Sup represent the probability that the quark of flavor Шаблон:Mvar decays into a quark of flavor Шаблон:Mvar. This 2×2 rotation matrix is called the "Cabibbo matrix", and was subsequently expanded to the 3×3 CKM matrix.

Файл:Quark weak interactions.svg

A pictorial representation of the six quarks' decay modes, with mass increasing from left to right.

CKM matrix

Файл:Weak Decay (flipped).svg

A diagram depicting the decay routes due to the charged weak interaction and some indication of their likelihood. The intensity of the lines is given by the CKM parameters

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]

<math>\begin{bmatrix} d' \\ s' \\ b' \end{bmatrix} = \begin{bmatrix} V_\mathrm{ud} & V_\mathrm{us} & V_\mathrm{ub} \\ V_\mathrm{cd} & V_\mathrm{cs} & V_\mathrm{cb} \\ V_\mathrm{td} & V_\mathrm{ts} & V_\mathrm{tb} \end{bmatrix} \begin{bmatrix} d \\ s \\ b \end{bmatrix}~.</math>

On the left are 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 flavour Шаблон:Mvar quark to another flavour Шаблон:Mvar quark. These transitions are proportional to |Шаблон:Mvar|Шаблон:Sup.

As of 2023, the best determination of the individual magnitudes of the CKM matrix elements was:^[6]

<math>

\begin{bmatrix} |V_{ud}| & |V_{us}| & |V_{ub}| \\ |V_{cd}| & |V_{cs}| & |V_{cb}| \\ |V_{td}| & |V_{ts}| & |V_{tb}| \end{bmatrix} = \begin{bmatrix} 0.97373 \pm 0.00031 & 0.2243 \pm 0.0008 & 0.00382 \pm 0.00020 \\ 0.221 \pm 0.004 & 0.975 \pm 0.006 & 0.0408 \pm 0.0014 \\ 0.0086 \pm 0.0002 & 0.0415 \pm 0.0009 & 1.014 \pm 0.029 \end{bmatrix}. </math>

Using those values, one can check the unitarity of the CKM matrix. In particular, we find that the first-row matrix elements give: <math> |V_\mathrm{ud}|^2 + |V_\mathrm{us}|^2 + |V_\mathrm{ub}|^2 = 0.9985 \pm 0.0007~;</math>

The difference from the theoretical value of 1 poses a tension of 2.2 standard deviations. Non-unitarity would be an indication of physics beyond the Standard Model.

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: The mass eigenstates Шаблон:Math, Шаблон:Math, and Шаблон:Math of the up-type quarks can equivalently define the matrix in terms of their weak interaction partners Шаблон:Math, Шаблон:Math, and Шаблон:Math. Since the CKM matrix is unitary, its inverse is the same as its conjugate transpose, which the alternate choices use; it appears as the same matrix, in a slightly altered form.

General case construction

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

An Шаблон:Sc × Шаблон:Sc unitary matrix (that is, a matrix Шаблон:Mvar such that Шаблон:Mvar, where Шаблон:Mvar is the conjugate transpose of Шаблон:Mvar and Шаблон:Mvar is the identity matrix) requires Шаблон:Sc² real parameters to be specified.
2Шаблон:Sc − 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 Шаблон:Sc² − (2Шаблон:Sc − 1) = (Шаблон:Sc − 1)².
- Of these, Шаблон:Sfrac Шаблон:Sc(Шаблон:Sc − 1) are rotation angles called quark mixing angles.
- The remaining Шаблон:Sfrac(Шаблон:Sc − 1)(Шаблон:Sc − 2) are complex phases, which cause CP violation.

Шаблон:Sc = 2

For the case Шаблон:Sc = 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.

Шаблон:Sc = 3

For the Standard Model case (Шаблон:Sc = 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 Шаблон:Nowrap Шаблон:Nowrap and Шаблон:Nowrap had similar amplitudes.
the transitions with change in strangeness Шаблон:Nowrap had amplitudes equal to Шаблон:Sfrac of those with Шаблон:Nowrap

Cabibbo's solution consisted of postulating weak universality (see below) to resolve the first issue, along with a mixing angle Шаблон:Math, now called the Cabibbo angle, between the Шаблон:Math and Шаблон:Math quarks to resolve the second.

For two generations of quarks, there can be no CP violating phases, as shown by the counting of the previous section. Since CP violations had already been seen in 1964, in neutral kaon decays, the Standard Model that emerged soon after clearly indicated the existence of a third generation of quarks, as Kobayashi and Maskawa pointed out in 1973. The discovery of the bottom quark at Fermilab (by Leon Lederman's group) in 1976 therefore immediately started off the search for the top quark, the missing third-generation quark.

Note, however, that the specific values that the angles take on are not a prediction of the standard model: They are free parameters. At present, there is no generally-accepted theory that explains why the angles should have the values that are measured in experiments.

Weak universality

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

separately for each generation Шаблон:Mvar. This implies that the sum of all couplings of any one 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

For any fixed and different Шаблон:Mvar and Шаблон:Mvar, this is a constraint on three complex numbers, one for each Шаблон:Mvar, which says that these numbers form the sides of a triangle in the complex plane. There are six choices of Шаблон:Mvar and Шаблон:Mvar (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 (introduced by Cecilia Jarlskog in 1985),

<math> J = c_{12}c_{13}^2 c_{23}s_{12}s_{13}s_{23}\sin \delta \approx 3\cdot10^{-5} ~.</math>

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

<math>(\beta,\alpha;i,j) = -(\alpha,\beta;i,j)=(\alpha,\beta;j,i) ~.</math>

Up to antisymmetry, it only has Шаблон:Nowrap non-vanishing components, which, remarkably, from the unitarity of Шаблон:Mvar, can be shown to be all identical in magnitude, that is,

<math>

(\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} \;, </math> so that

<math>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) ~.</math>

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.

Parameterizations

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

<math>\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}. </math>

"Standard" parameters

A "standard" parameterization of the CKM matrix uses three Euler angles (Шаблон:Thin space Шаблон:Mvar Шаблон:Sub, Шаблон:Mvar Шаблон:Sub, Шаблон:Mvar Шаблон:Sub Шаблон:Thin space) and one CP-violating phase (Шаблон:Thin space Шаблон:Mvar Шаблон:Sub Шаблон:Thin space).^[8] Шаблон:Mvar Шаблон:Sub is the Cabibbo angle. Couplings between quark generations Шаблон:Math and Шаблон:Math vanish if Шаблон:Nowrap. Cosines and sines of the angles are denoted Шаблон:Mvar Шаблон:Sub and Шаблон:Mvar Шаблон:Sub, respectively.

<math> \begin{align} & \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{align} </math>

The 2008 values for the standard parameters were:^[9]

Шаблон:Mvar Шаблон:Sub = Шаблон:Val, Шаблон:Mvar Шаблон:Sub = Шаблон:Val, Шаблон:Mvar Шаблон:Sub = Шаблон:Val

and

Шаблон:Mvar Шаблон:Sub = Шаблон:Val radians = Шаблон:Val.

Wolfenstein parameters

A third parameterization of the CKM matrix was introduced by Lincoln Wolfenstein with the four parameters Шаблон:Mvar, Шаблон:Mvar, Шаблон:Mvar, and Шаблон:Mvar, which would all 'vanish' (would be zero) if there were no coupling.^[10] The four Wolfenstein parameters have the property that all are of order 1 and are related to the 'standard' parameterization:

<math> \lambda = s_{12} ~, </math>	<math> \lambda = s_{12} ~,</math>
<math> A \lambda^2 = s_{23} ~, </math>	<math> A = \frac{s_{23} }{\; s_{12}^2 \;} ~,</math>
<math> A \lambda^3 ( \rho - i \eta ) = s_{13} e^{-i\delta} ~, \quad </math>	<math> \rho = \operatorname\mathcal{R_e} \left\{ \frac{\; s_{13} \, e^{-i\delta} \;}{ s_{12} \, s_{23} } \right\} ~, \quad \eta = - \operatorname\mathcal{I_m} \left\{ \frac{\; s_{13} \, e^{-i\delta} \;}{ s_{12} \, s_{23} } \right\} ~. </math>

Although the Wolfenstein parameterization of the CKM matrix can be as exact as desired when carried to high order, it is mainly used for generating convenient approximations to the standard parameterization. The approximation to order Шаблон:Mvar Шаблон:Sup, good to better than 0.3% accuracy, is:

<math>\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) ~. </math>

Rates of CP violation correspond to the parameters Шаблон:Mvar and Шаблон:Mvar.

Using the values of the previous section for the CKM matrix, as of 2008 the best determination of the Wolfenstein parameter values is:^[11]

Шаблон:Mvar = Шаблон:Val, Шаблон:Mvar = Шаблон:Val, Шаблон:Mvar = Шаблон:Val, and Шаблон:Mvar = Шаблон:Val.

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]

References

Шаблон:Reflist

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Английская Википедия:Cabibbo–Kobayashi–Maskawa matrix

Содержание

The matrix

Predecessor – the Cabibbo matrix

CKM matrix

General case construction

Шаблон:Sc = 2

Шаблон:Sc = 3

Observations and predictions

Weak universality

The unitarity triangles

Parameterizations

KM parameters

"Standard" parameters

Wolfenstein parameters

Nobel Prize

See also

References

Further reading and external links

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