CPT theorem

E645109

The CPT theorem is a fundamental result in quantum field theory stating that any Lorentz-invariant local quantum field theory with a Hermitian Hamiltonian is invariant under the combined operations of charge conjugation (C), parity transformation (P), and time reversal (T).

All labels observed (2)

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Statements (51)

Predicate Object
instanceOf symmetry principle ⓘ
theorem in quantum field theory ⓘ
abbreviation CPT theorem ⓘ
allows violation of C symmetry alone ⓘ
violation of CP symmetry ⓘ
violation of CT symmetry ⓘ
violation of P symmetry alone ⓘ
violation of PT symmetry ⓘ
violation of T symmetry alone ⓘ
appliesTo free quantum field theories ⓘ
interacting quantum field theories ⓘ
relativistic quantum field theories ⓘ
constrains possible violations of discrete symmetries in quantum field theory ⓘ
field quantum field theory ⓘ
forbids violation of combined CPT symmetry in local Lorentz-invariant QFT ⓘ
fullName charge conjugation–parity–time reversal theorem ⓘ
linked to: CPT theorem
hasMathematicalFramework Wightman axioms ⓘ
axiomatic quantum field theory ⓘ
historicallyProvedBy Gerhard Lüders ⓘ
Julian Schwinger ⓘ
Wolfgang Pauli ⓘ
holdsIn Minkowski spacetime ⓘ
implies equality of magnitudes of particle and antiparticle charges with opposite sign ⓘ
equality of particle and antiparticle lifetimes ⓘ
equality of particle and antiparticle masses ⓘ
existence of antiparticles with related properties to particles ⓘ
impliesInvarianceUnder combined CPT transformation ⓘ
involvesOperation charge conjugation ⓘ
parity transformation ⓘ
time reversal ⓘ
isConsequenceOf Lorentz invariance and locality in Minkowski spacetime ⓘ
microcausality ⓘ
unitarity ⓘ
isRelatedTo Lorentz symmetry ⓘ
linked to: Lorentz group

Poincaré invariance ⓘ
discrete symmetries in quantum field theory ⓘ
spin–statistics theorem ⓘ
isTestedBy B-meson experiments ⓘ
kaon experiments ⓘ
neutral meson systems ⓘ
precision spectroscopy of particles and antiparticles ⓘ
isUsedIn high-energy physics experiments ⓘ
particle physics ⓘ
tests of fundamental symmetries ⓘ
mayFailIf Hamiltonian is non-Hermitian ⓘ
Lorentz invariance is violated ⓘ
locality is violated ⓘ
requiresProperty Hermitian Hamiltonian ⓘ
Lorentz invariance ⓘ
locality ⓘ
states any Lorentz-invariant local quantum field theory with a Hermitian Hamiltonian is invariant under CPT ⓘ

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Referenced by (4)

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

Sakharov conditions → relatesTo → CPT theorem ⓘ
CPT theorem → fullName → charge conjugation–parity–time reversal theorem ⓘ
linked to: CPT theorem
CPT theorem → abbreviation → CPT theorem ⓘ