Two- and four-dimensional representations of the PT- and CPT -symmetric fermionic algebras

Fermionic systems differ from their bosonic counterparts, the main difference with regard to symmetry considerations being that T2=−1 for fermionic systems. In PT-symmetric quantum mechanics an operator has both PT and CPT adjoints. Fermionic operators η, which are quadratically nilpotent (η2=0), an...

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Bibliographic Details
Main Authors: Beygi, Alireza (Author) , Klevansky, Sandra Pamela (Author) , Bender, Carl M. (Author)
Format: Article (Journal)
Language:English
Published: 28 March 2018
In: Physical review
Year: 2018, Volume: 97, Issue: 3
ISSN:2469-9934
DOI:10.1103/PhysRevA.97.032128
Online Access:Verlag, Volltext: http://dx.doi.org/10.1103/PhysRevA.97.032128
Verlag, Volltext: https://link.aps.org/doi/10.1103/PhysRevA.97.032128
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Author Notes:Alireza Beygi, S.P. Klevansky, and Carl M. Bender
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Two- and four-dimensional representations of the PT- and CPT-symmetric fermionic algebras by Beygi, Alireza (Author) , Klevansky, Sandra Pamela (Author) , Bender, Carl M. (Author) ,


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