neutral kaon system

E543037

The neutral kaon system is a quantum two-state system of strange mesons whose weak-interaction mixing and CP-violating behavior make it a key testing ground for fundamental symmetries in particle physics.

All labels observed (1)

Label Occurrences
neutral kaon system canonical 1

How this entity was disambiguated

Statements (50)

Predicate Object
instanceOf CP-violating system ⓘ
flavor oscillation system ⓘ
meson system ⓘ
quantum two-state system ⓘ
testbed for fundamental symmetries ⓘ
consistsOf K0 meson ⓘ
anti-K0 meson ⓘ
decaysVia semileptonic decays ⓘ
three-pion final states ⓘ
two-pion final states ⓘ
exhibits CP violation ⓘ
T violation ⓘ
direct CP violation ⓘ
indirect CP violation ⓘ
hasApproximateSymmetry CP symmetry in the limit ε → 0 ⓘ
hasComponent K0 (down anti-strange) ⓘ
anti-K0 (strange anti-down) ⓘ
hasEffectiveEigenstate KL (long-lived neutral kaon) ⓘ
linked to: neutral kaon mixing

KS (short-lived neutral kaon) ⓘ
hasObservable CP-violating parameter epsilon (ε) ⓘ
decay width difference ΔΓ between KS and KL ⓘ
direct CP-violating parameter epsilon-prime (ε′) ⓘ
mass difference Δm between KS and KL ⓘ
hasProperty flavor eigenstates differ from mass eigenstates ⓘ
mass eigenstates KS and KL have different lifetimes ⓘ
mass eigenstates KS and KL have slightly different masses ⓘ
non-Hermitian effective Hamiltonian for decays ⓘ
hasQuantumNumber isospin I = 1/2 ⓘ
spin 0 ⓘ
strangeness S = +1 for K0 ⓘ
strangeness S = −1 for anti-K0 ⓘ
hasTheoreticalTool density matrix formalism for decoherence studies ⓘ
isDescribedBy Weisskopf–Wigner approximation ⓘ
effective 2×2 Hamiltonian formalism ⓘ
standard model of particle physics ⓘ
isGovernedBy electromagnetic interaction (for some decays) ⓘ
strong interaction (for production and hadronization) ⓘ
weak interaction ⓘ
isPrototypeFor other neutral meson mixing systems (Bd, Bs, D0, B0s) ⓘ
isUsedIn precision tests of quantum mechanics ⓘ
searches for physics beyond the standard model ⓘ
isUsedToTest CP symmetry ⓘ
CPT symmetry ⓘ
T symmetry ⓘ
unitarity of the CKM matrix ⓘ
ΔS = ΔQ rule in weak decays ⓘ
undergoes K0–anti-K0 mixing ⓘ
wasCentralTo discovery of CP violation in 1964 ⓘ
wasStudiedAt Brookhaven National Laboratory ⓘ
CERN kaon experiments ⓘ

How these facts were elicited

Referenced by (1)

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

K-short → isMassEigenstateOf → neutral kaon system ⓘ