Cabibbo–Kobayashi–Maskawa matrix

E234496

The Cabibbo–Kobayashi–Maskawa matrix is a fundamental component of the Standard Model of particle physics that describes how quarks change flavor via the weak interaction and accounts for CP violation in the quark sector.

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All labels observed (5)

Statements (50)

Predicate Object
instanceOf concept in the Standard Model of particle physics
flavor mixing matrix
unitary matrix
accountsFor CP violation in the quark sector
appliesTo down, strange, bottom quarks
three generations of quarks
up, charm, top quarks
constrains unitarity triangles
describes charged-current weak interaction couplings of quarks
quark flavor mixing
quark mixing in weak interactions
generalizes Cabibbo angle description of quark mixing
hasApproximateMagnitudePattern |V_cb|, |V_ts| of order 0.04
|V_ub|, |V_td| much smaller than 1
|V_ud|, |V_cs|, |V_tb| close to 1
|V_us|, |V_cd| of order 0.22
hasDimension 3×3
hasElement V_cb
V_cd
V_cs
V_tb
V_td
V_ts
V_ub
V_ud
V_us
hasParameter one CP-violating phase
three mixing angles
hasParameterization Wolfenstein parameterization
standard PDG parameterization
hasProperty complex phases
nontrivial CP-violating phase
unitarity
introducedBy Makoto Kobayashi NERFINISHED
Nicola Cabibbo
Toshihide Maskawa
namedAfter Makoto Kobayashi NERFINISHED
Nicola Cabibbo
Toshihide Maskawa
partOf Standard Model
surface form: Standard Model of particle physics
relatedTo Cabibbo–Kobayashi–Maskawa matrix self-linksurface differs
surface form: Jarlskog invariant
relates down-type quarks
mass eigenstates of quarks
up-type quarks
weak interaction eigenstates of quarks
symbol V_CKM
usedIn B meson physics
D meson physics
K meson physics
calculation of weak decay rates of hadrons

How these facts were elicited

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Instruction
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Input
Subject: Cabibbo–Kobayashi–Maskawa matrix
Description of subject: The Cabibbo–Kobayashi–Maskawa matrix is a fundamental component of the Standard Model of particle physics that describes how quarks change flavor via the weak interaction and accounts for CP violation in the quark sector.

Referenced by (16)

Full triples — surface form annotated when it differs from this entity's canonical label.

Toshihide Maskawa knownFor Cabibbo–Kobayashi–Maskawa matrix
Toshihide Maskawa knownFor Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: CKM matrix
GIM mechanism relatedTo Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: Cabibbo angle
GIM mechanism relatedTo Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: CKM matrix
Makoto Kobayashi contributedTo Cabibbo–Kobayashi–Maskawa matrix
Cabibbo–Kobayashi–Maskawa matrix relatedTo Cabibbo–Kobayashi–Maskawa matrix self-linksurface differs
this entity surface form: Jarlskog invariant
Kobayashi–Maskawa theory usesConcept Cabibbo–Kobayashi–Maskawa matrix
Kobayashi–Maskawa theory usesConcept Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: CKM matrix
Kobayashi–Maskawa theory relatedConcept Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: Jarlskog invariant
Kobayashi–Maskawa paper on CP violation (1973) mainSubject Cabibbo–Kobayashi–Maskawa matrix
Kobayashi–Maskawa paper on CP violation (1973) laterCalled Cabibbo–Kobayashi–Maskawa matrix
Kobayashi–Maskawa paper on CP violation (1973) relatedConcept Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: CKM matrix
Maskawa knownFor Cabibbo–Kobayashi–Maskawa matrix
subject surface form: Makoto Kobayashi
Maskawa coAuthorOf Cabibbo–Kobayashi–Maskawa matrix
subject surface form: Makoto Kobayashi
this entity surface form: Cabibbo–Kobayashi–Maskawa theory
Maskawa notableConcept Cabibbo–Kobayashi–Maskawa matrix
subject surface form: Makoto Kobayashi
this entity surface form: CKM matrix
Yukawa coupling relatedTo Cabibbo–Kobayashi–Maskawa matrix
this entity surface form: CKM matrix