theorem

CPT theorem

The CPT theorem states that any Lorentz-invariant quantum field theory is invariant under the combined operations of charge conjugation, parity, and time reversal.
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Description

The CPT theorem is one of the cornerstones of modern quantum field theory. Its origins lie in the works of Julian Schwinger, Wolfgang Pauli, and Gerhart Lüders, who in the 1950s showed that the combination of three discrete symmetries must be an exact symmetry of any local relativistic field. Later, John Stewart Bell and others gave more general proofs. Despite the fact that weak interactions violate both parity (P) and charge conjugation (C), and even the CP combination, CPT remains unbroken — so far not a single experimental hint of its violation has been found.

History

The theorem was gradually formulated in the 1950s. In 1951, Julian Schwinger showed the connection between CPT and spin-statistics. In 1954, Gerhart Lüders derived CPT invariance within the general approach of quantum field theory. Wolfgang Pauli in 1955 proposed the famous proof and gave the theorem its name. John Stewart Bell in the 1960s generalized the results. Since then, the CPT theorem has been tested in experiments with the highest precision, for example, in antihydrogen experiments at CERN.

How it works

CPT invariance is used for classifying elementary particles and predicting properties of their antipartners. In accelerators, when particle-antiparticle pairs are created, CPT guarantees strict kinematic relations. Experimental limits on CPT violation are ultrasensitive: the relative mass difference between K0-meson and its antiparticle is less than 10^-18. Limits of applicability — within Lorentz-invariant quantum field theory; in theories with Lorentz invariance violation (for example, quantum gravity) CPT may be violated.

In practice

Guarantees that any particle has an antiparticle with exactly the same mass and lifetime; without this theorem, there would be no predictions of antimatter properties.

Fun fact

If CPT symmetry were violated even slightly, particles and antiparticles could have slightly different masses, which might explain why there is much more matter than antimatter in the Universe. But so far all measurements show complete symmetry.

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