Both sides previous revision Previous revision Next revision | Previous revision | ||
theorems:cpt [2018/04/16 17:39] jakobadmin [Concrete] |
theorems:cpt [2018/05/05 12:23] (current) jakobadmin ↷ Links adapted because of a move operation |
||
---|---|---|---|
Line 15: | Line 15: | ||
* The canonical commutation or anti-commutation rules hold for the fields. | * The canonical commutation or anti-commutation rules hold for the fields. | ||
- | Formulated differently, the CPT theorem says that any Lorentz invariant local [[theories:quantum_field_theory|quantum field theory]] with a Hermitian Hamiltonian must be CPT symmetric. | + | Formulated differently, the CPT theorem says that any Lorentz invariant local [[theories:quantum_field_theory:canonical|quantum field theory]] with a Hermitian Hamiltonian must be CPT symmetric. |
From these assumptions it follows that the Lagrangian is also invariant under the produce of C, P, and T , taken in any order. Take note that $C$, $P$, $T$ or any other product of them can be violated, which CPT is intact. This means concretely that we can always choose the phases which appear in C, P, T transformations such that the product of those operators is a symmetry of our theory. | From these assumptions it follows that the Lagrangian is also invariant under the produce of C, P, and T , taken in any order. Take note that $C$, $P$, $T$ or any other product of them can be violated, which CPT is intact. This means concretely that we can always choose the phases which appear in C, P, T transformations such that the product of those operators is a symmetry of our theory. | ||
Line 22: | Line 22: | ||
component transformations. | component transformations. | ||
+ | To test the CPT symmetry we compare the masses, lifetimes, electric charges and anomalous magnetic | ||
+ | moments of particles with their corresponding antiparticles. Another possibility are detailed analysis of the behaviour of neutral flavoured meson systems. | ||
+ | ---- | ||
+ | |||
+ | * For a nice discussion see Chapter 5 in “Discrete Symmetries and CP Violation: From Experiment to Theory” by Marco Sozzi | ||