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For theoretical discussions of Lorentz violation in electrodynamics see, for example, R. Jackiw and V. A. Kostelecký, Phys. Rev. Lett. 82, 3572 (1999); M. Pérez-Victoria, J. High Energy Phys. 04 (2001) 032; V. A. Kostelecký, C. D. Lane, and A. G. M. Pickering, Phys. Rev. D 65, 056006 (2002); C. Adam and F. R. Klinkhamer, Nucl. Phys. B657, 214 (2003); H. Müller et al., Phys. Rev. D 67, 056006 (2003); T. Jacobson, S. Liberati, and D. Mattingly, Phys. Rev. D 67, 124011 (2003); V. A. Kostelecký and A. G. M. Pickering, Phys. Rev. Lett. 91, 031 801 (2003); R. Lehnert, Phys. Rev. D 68, 085003 (2003); G. M. Shore, Contemp. Phys. 44, 503 (2003); B. Altschul, Phys. Rev. D 69, 125009 (2004); Phys. Rev. D 70, 101701 (2004); hep-th/0402036; T. Jacobson, S. Liberati, D. Mattingly, and F. Stecker, Phys. Rev. Lett. 93, 021101 (2004); R. Lehnert and R. Potting, Phys. Rev. Lett. 93, 110 402 (2004); Phys. Rev. D 70, 125010 (2004); Phys. Rev. D 70, 129906(E) (2004); F. R. Klinkhamer and C. Rupp, Phys. Rev. D 70, 045020 (2004); Q. Bailey and V. A. Kostelecký, Phys. Rev. D 70, 076006 (2004); C. Lämmerzahl, A. Macias, and H. Müller, Phys. Rev. D 71, 025007 (2005); C. Lämmerzahl and F. W. Hehl, Phys. Rev. D 70, 105022 (2004); H. Belich, T. Costa-Soares, M. M. Ferreira, and J. A. Helayel-Neto, hep-th/0411151.
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CPT is a discrete symmetry, so no new NG modes accompany its spontaneous breaking. The NG modes for Lorentz violation are, however, expected to be present if CPT is broken because CPT violation is accompanied by Lorentz violation in conventional field theories. See O. W. Greenberg, Phys. Rev. Lett. 89, 231 602 (2002); Phys. Lett. B 567, 179 (2003).
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CPT is a discrete symmetry, so no new NG modes accompany its spontaneous breaking. The NG modes for Lorentz violation are, however, expected to be present if CPT is broken because CPT violation is accompanied by Lorentz violation in conventional field theories. See O. W. Greenberg, Phys. Rev. Lett. 89, 231 602 (2002); Phys. Lett. B 567, 179 (2003).
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Phys. Lett. B
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note
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Under special circumstances more than 10 generators are involved. For example, in a theory based on special relativity with multiple noninteracting particle species, there are distinct particle Lorentz transformations for each field. The particle symmetry group of the theory then contains a direct product of several Lorentz groups, and so there could be multiple sets of NG modes. However, in typical gravitational theories with the metric coupling to all irreducible tensors, the full particle invariance involves only one copy of the particle Lorentz and diffeomorphism groups, so only ten corresponding NG modes can appear.
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Models with this kinetic term have been considered in J. W. Moffat, Int. J. Mod. Phys. D 2, 351 (1993); Found. Phys. 23, 411 (1993).
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Note that, in a Lorentz-invariant theory only, the effects of the particle transformations considered in this subsection are equivalent in their action on tensor components to certain inverse observer transformations. The Minkowskispacetime transformations (36) then correspond to observer Lorentz transformations to a local frame with an anholonomic basis, and the diffeomorphisms leading to Eq. (38) correspond to working with special relativity in a non-Cartesian basis.
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155
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0036576493
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This result can be traced to unobservable field redefinitions that eliminate certain coefficients for Lorentz violation. See Refs. [5,7,24] and M. S. Berger and V. A. Kostelecký, Phys. Rev. D 65, 091701(R) (2002); D. Colladay and P. McDonald, J. Math. Phys. (N.Y.) 43, 3554 (2002).
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This result can be traced to unobservable field redefinitions that eliminate certain coefficients for Lorentz violation. See Refs. [5,7,24] and M. S. Berger and V. A. Kostelecký, Phys. Rev. D 65, 091701(R) (2002); D. Colladay and P. McDonald, J. Math. Phys. (N.Y.) 43, 3554 (2002).
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