Projective geometry and PT-symmetric Dirac Hamiltonian
@article{Ng2009ProjectiveGA, title={Projective geometry and PT-symmetric Dirac Hamiltonian}, author={Y. J. Ng and H. V. Dam}, journal={Physics Letters B}, year={2009}, volume={673}, pages={237-239} }
Abstract The ( 3 + 1 )-dimensional (generalized) Dirac equation is shown to have the same form as the equation expressing the condition that a given point lies on a given line in 3-dimensional projective space. The resulting Hamiltonian with a γ 5 mass term is not Hermitian, but is invariant under the combined transformation of parity reflection P and time reversal T . When the PT symmetry is unbroken, the energy spectrum of the free spin- 1 2 theory is real, with an appropriately shifted mass.
One Citation
Non-Hermitian non-PT-symmetric Dirac Hamiltonians with real energy eigenvalues
- Physics, Mathematics
- 2013
- 3
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References
SHOWING 1-10 OF 13 REFERENCES
Phys
- Lett. B625, 333
- 2005
Phys
- Rev. Lett. 80, 5243 (1998). Also see C. M. Bender and K. A. Milton, Phys. Rev. D 55, 3255
- 1997
Rept
- Prog. Phys. 70, 947
- 2007
The idea of PT symmetry was prefigured in the latter paper . [ 2 ] C . M . Bender , Rept
- Prog . Phys .
- 2007
Proc
- Nat. Acad. Sci. USA, 19, 503 (1933); E. M. Bruins, Proc. Nederl. Akad. Wetensch. 52, 1135 (1949); F. C. Taylor Jr., Master thesis, University of North Carolina at Chapel Hill
- 1968