Quantization in a non-microcausal field theory.
It was first shown by Pauli 1) that from the requirement of Lorentz invariance, microcausality and positive energy and of the assumption that either commutators or anticommutators are c-numbers we must quantize, for the case of free field, half-integer spin field with Fermi-Dirac statistics and inte...
| Main Author: | |
|---|---|
| Other Authors: | |
| Format: | Others |
| Language: | en |
| Published: |
McGill University
1966
|
| Subjects: | |
| Online Access: | http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=43760 |
| Summary: | It was first shown by Pauli 1) that from the requirement of Lorentz invariance, microcausality and positive energy and of the assumption that either commutators or anticommutators are c-numbers we must quantize, for the case of free field, half-integer spin field with Fermi-Dirac statistics and integral spin field with Bose-Einstein statistics. [...] |
|---|