V_cb

E815591

V_cb is the CKM matrix element that quantifies the strength of quark flavor-changing transitions between charm and bottom quarks in the Standard Model of particle physics.

All labels observed (1)

Label Occurrences
V_cb canonical 1

How this entity was disambiguated

Statements (47)

Predicate Object
instanceOf CKM matrix element ⓘ
complex number ⓘ
affects predictions for B meson lifetimes and branching ratios ⓘ
rates of rare B decays via normalization of b → c transitions ⓘ
appearsIn W boson couplings to quarks ⓘ
charged-current weak interactions ⓘ
approximatelyEquals A λ² in Wolfenstein parametrization ⓘ
constrainedBy unitarity of the CKM matrix ⓘ
constrains models of new physics affecting b → c transitions ⓘ
contributesTo determination of CKM unitarity triangle ⓘ
dependsOn hadronic form factors ⓘ
describes quark flavor-changing transitions between charm and bottom quarks ⓘ
dimension dimensionless ⓘ
expressedIn Wolfenstein parametrization of the CKM matrix ⓘ
governs b → c transitions ⓘ
b̄ → c̄ transitions ⓘ
hasApproximateMagnitude 0.04 ⓘ
|V_cb| ≈ 4 × 10⁻² ⓘ
hasPhaseConvention can be chosen approximately real in standard CKM phase convention ⓘ
hasRole input parameter in precision flavor physics ⓘ
hasUncertaintySource experimental systematics ⓘ
theoretical form-factor calculations ⓘ
hierarchyProperty |V_cb| ≪ |V_cs| and |V_cb| ≪ |V_tb| ⓘ
|V_cb| ≫ |V_ub| ⓘ
isSubjectOf heavy quark effective theory analyses ⓘ
inclusive–exclusive determination tension studies ⓘ
lattice QCD calculations ⓘ
matrixPosition row corresponding to charm quark, column corresponding to bottom quark ⓘ
measuredIn exclusive B → D ℓ ν decays ⓘ
exclusive B → D* ℓ ν decays ⓘ
inclusive b → c ℓ ν decays ⓘ
semileptonic B meson decays ⓘ
namedAfter Cabibbo ⓘ
Kobayashi ⓘ
Maskawa ⓘ
parameterOf weak interaction Lagrangian ⓘ
partOf Cabibbo–Kobayashi–Maskawa matrix ⓘ
Standard Model of particle physics ⓘ
linked to: Standard Model
relatedTo V_ub via CKM hierarchy ⓘ
Wolfenstein parameter A ⓘ
relatesQuarkFlavor bottom quark ⓘ
charm quark ⓘ
symbolFor CKM element between second and third quark generations ⓘ
usedIn global CKM fits ⓘ
normalization of b → c semileptonic spectra ⓘ
tests of CKM unitarity in the second and third columns ⓘ
usedToDetermine strength of b → c weak transitions ⓘ

How these facts were elicited

Referenced by (1)

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