Abstract
A non-local field theory that breaks discrete symmetries, including C, P, CP, and CPT, but preserves Lorentz symmetry, is presented. We demonstrate that at one-loop level the masses for particle and antiparticle remain equal due to Lorentz symmetry only. An inequality of masses implies breaking of the Lorentz invariance and non-conservation of the usually conserved charges.
Similar content being viewed by others
References
H. Murayama and T. Yanagida, Phys. Lett. B 520, 263 (2001).
G. Barenboim, L. Borissov, J. D. Lykken, and A. V. Smirnov, J. High Energy Phys. 0210, 001 (2002); G. Barenboim, L. Borissov, and J. D. Lykken, Phys. Lett. B 534, 106 (2002); G. Barenboim, J. F. Beacom, L. Borissov, and B. Kayser, Phys. Lett. B 537, 227 (2002); G. Barenboim, L. Borissov, and J. D. Lykken, hep-ph/0212116.
O. W. Greenberg, Phys. Rev. Lett. 89, 231602 (2002).
M. Chaichian, A. D. Dolgov, V. A. Novikov, and A. Tureanu, Phys. Lett. B 699, 177 (2011).
A. D. Dolgov, Phys. At. Nucl. 73, 588 (2010); arXiv:0903.4318 [hep-ph].
M. Chaichian, K. Fujikawa, and A. Tureanu, hepth/1203.0267.
M. B. Voloshin and L. B. Okun, JETP Lett. 28, 145 (1978).
Author information
Authors and Affiliations
Additional information
The article is published in the original.
Rights and permissions
About this article
Cite this article
Dolgov, A.D., Novikov, V.A. CPT, Lorentz invariance, mass differences, and charge non-conservation. Jetp Lett. 95, 594–597 (2012). https://doi.org/10.1134/S0021364012110033
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1134/S0021364012110033