CPT symmetry is recognized to be a fundamental property of physical laws.

This is a major class of experimental tests of CPT symmetry.

CPT symmetry neither requires nor rules out a physical actualization of that symmetry.

CPT symmetry is a basic consequence of quantum field theory and no violations of it have ever been detected.

By CPT symmetry, there is a set of right-handed fermions with the opposite quantum numbers.

Thus, this CPT symmetry ensures the same self-attractive gravitational behavior for both matter and antimatter.

CPT symmetry (combining charge, parity and time conjugation)

Only a weaker version of the symmetry could be preserved by physical phenomena, which was CPT symmetry.

It investigates possible spontaneous breaking of both Lorentz invariance and CPT symmetry.

Modern physics is not quite time-reversible; instead it exhibits a broader symmetry, CPT symmetry.

CPT symmetry doesn't imply that our universe makes use of that symmetry, but it's a suggestive connection nevertheless.

This would violate CPT symmetry and Lorentz symmetry.

Having also CPT symmetry, the combined symmetry CP is violated as well.

Second, in microphysics of weak interaction the T-symmetry may be violated and only the combined CPT symmetry holds.

Furthermore, due to CPT symmetry reversal of time direction is equivalent to renaming particles as antiparticles and vice versa.

Besides the confirmation of time dilation, also CPT symmetry was confirmed by comparing the lifetimes of positive and negative particles.

In the early 1990s, it was shown in the context of bosonic superstrings that string interactions can also spontaneously break CPT symmetry.

The magnitude of properties of the antiproton are predicted by CPT symmetry to be exactly related to those of the proton.

Finally, the interactions must be out of thermal equilibrium, since otherwise CPT symmetry would assure compensation between processes increasing and decreasing the baryon number.

Full details of the general formalism for Lorentz and CPT symmetry in the neutrino sector appeared in a 2004 publication.

CPT symmetry is a fundamental symmetry of physical laws under transformations that involve the simultaneous inversion of charge, parity, and time.

The CPT theorem requires the preservation of CPT symmetry by all physical phenomena.

CPT symmetry must be preserved in any Lorentz invariant local quantum field theory with a Hermitian Hamiltonian.

Then , so a test of CPT symmetry is that the masses and the decay widths of the particle and the antiparticle are equal.

In their paper the authors already consider non-invariance under T (time reversal) and hence, given the assumption of CPT symmetry, also under CP.