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P,T,PT, and CPT invariance of Hermitian Hamiltonians
Quantum Physics · Submitted 11 Feb 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We propose generalized definitions of time-reversal operator (T) and orthonormality such that all Hermitian Hamiltonians are P, T, PT, and CPT invariant.
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The abstract, sentence by sentence
Currently, it has been claimed that certain Hermitian Hamiltonians have parity (P) and they are PT-invariant. We propose generalized definitions of time-reversal operator (T) and orthonormality such that all Hermitian Hamiltonians are P, T, PT, and CPT invariant. The PT-norm and CPT-norm are indefinite and definite respectively. The energy-eigenstates are either E-type (e.g., even) or O-type (e.g., odd). C mimics the charge-conjugation symmetry which is recently found to exist for a non-Hermitian Hamiltonian. For a Hermitian Hamiltonian it coincides with P.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Currently, it has been claimed that certain Hermitian Hamiltonians have parity (P) and they are PT-invariant. | background 0.99 | 0.04 | 0.04 | asserted 0.93 |
| s1 | We propose generalized definitions of time-reversal operator (T) and orthonormality such that all Hermitian Hamiltonians are P, T, PT, and CPT invariant. | contribution 0.99 | 0.89 | 0.80 | asserted 0.84 |
| s2 | The PT-norm and CPT-norm are indefinite and definite respectively. | result 0.98 | 0.71 | 0.10 | asserted 1.00 |
| s3 | The energy-eigenstates are either E-type (e.g., even) or O-type (e.g., odd). | result 0.87 | 0.73 | 0.06 | asserted 1.00 |
| s4 | C mimics the charge-conjugation symmetry which is recently found to exist for a non-Hermitian Hamiltonian. | background 0.47 | 0.15 | 0.04 | asserted 0.98 |
| s5 | For a Hermitian Hamiltonian it coincides with P. | result 0.88 | 0.51 | 0.07 | asserted 1.00 |
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Original abstract
Currently, it has been claimed that certain Hermitian Hamiltonians have parity (P) and they are PT-invariant. We propose generalized definitions of time-reversal operator (T) and orthonormality such that all Hermitian Hamiltonians are P, T, PT, and CPT invariant. The PT-norm and CPT-norm are indefinite and definite respectively. The energy-eigenstates are either E-type (e.g., even) or O-type (e.g., odd). C mimics the charge-conjugation symmetry which is recently found to exist for a non-Hermitian Hamiltonian. For a Hermitian Hamiltonian it coincides with P.
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