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3
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see also E731 Collaboration, L. K. Gibbons, Phys. Rev. D 55, 6625 (1997)
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85037254002
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CPLEAR Collaboration, P. Kokkas, presented at the Conference on High Energy Physics, Vancouver, 1998;, P. Bloch, presented at the KAON 99 Conference, Chicago, 1999
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CPLEAR Collaboration, P. Kokkas, presented at the Conference on High Energy Physics, Vancouver, 1998;P. Bloch, presented at the KAON 99 Conference, Chicago, 1999.
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7
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World Scientific, Singapore, G. Diambrini-Palazzi, C. Cosmelli, L. Zanello
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Franzini, P.1
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See, for example, C. Bhat et al., Report FERMILAB-P-0894 (1998)
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See, for example, C. Bhat et al., Report FERMILAB-P-0894 (1998).
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OPAL Collaboration, R. Ackerstaff, Z. Phys. C 76, 401 (1997).
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DELPHI Collaboration, M. Feindt et al., Report DELPHI 97-98 CONF 80 (1997)
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DELPHI Collaboration, M. Feindt et al., Report DELPHI 97-98 CONF 80 (1997).
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12
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85037235683
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A number of recent theoretical efforts along these lines are discussed in CPT and Lorentz Symmetry, edited by V. A. Kostelecký (World Scientific, Singapore, 1999)
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A number of recent theoretical efforts along these lines are discussed in CPT and Lorentz Symmetry, edited by V. A. Kostelecký (World Scientific, Singapore, 1999).
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13
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85037202549
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A discussion of the discrete symmetries C, P, T, and their combinations can be found in R. G. Sachs, The Physics of Time Reversal (University of Chicago Press, Chicago, 1987)
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A discussion of the discrete symmetries C, P, T, and their combinations can be found in R. G. Sachs, The Physics of Time Reversal (University of Chicago Press, Chicago, 1987).
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14
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World Scientific, Singapore, C. Jarlskog
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CP Violation, edited by C. Jarlskog (World Scientific, Singapore, 1989).
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H. Dehmelt, Phys. Rev. Lett. (to be published), hep-ph/9906262.
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It has been suggested that in the kaon system CPT-violating effects might be generated through an unconventional quantum mechanics in which the Schrödinger equation is replaced with a density-matrix formalism. See J. Ellis, Phys. Rev. D 53, 3846 (1996), where it is also shown that the resulting effects can be disentangled from the CPT-violating parameter (Formula presented) of interest here.
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Ellis, J.1
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Direct CPT violation in the decay amplitudes is neglected here because it is suppressed in the standard-model extension and is expected to be unobservable
-
Direct CPT violation in the decay amplitudes is neglected here because it is suppressed in the standard-model extension and is expected to be unobservable 14.
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63
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85037254016
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A field redefinition can be used to shift equally the values of all the parameters (Formula presented) without physical consequences
-
A field redefinition can be used to shift equally the values of all the parameters (Formula presented) without physical consequences 15. For a particular (Formula presented) meson, one could therefore replace (Formula presented) with a single (Formula presented) factor. For clarity, this redefinition is avoided in the present work.
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65
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Some authors have suggested a relatively large momentum dependence for T violation: J. S. Bell and J. K. Perring, Phys. Rev. Lett. 13, 348 (1964)
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R. M. Green, Spherical Astronomy (Cambridge University Press, Cambridge, England, 1985).
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85037237508
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KTeV Collaboration, A. Alavi-Harati et al., Report EFI 99-25 (1999)
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KTeV Collaboration, A. Alavi-Harati et al., Report EFI 99-25 (1999)
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72
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see also NA31 Collaboration, G. D. Barr, Phys. Lett. B 317, 233 (1993)
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Barr, G.D.1
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75
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0000350283
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A careful analysis involving the use of the magnitude and phase of (Formula presented) and (Formula presented) can yield a CPT test, but it is necessary to account for contributions to the effective Hamiltonian arising from 3π decays and from violations of the (Formula presented) rule in semileptonic decays. See L. Lavoura, Mod. Phys. Lett. A 7, 1367 (1992).
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Lavoura, L.1
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79
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85037251717
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KTeV Collaboration, presented by Y. B. Hsiung at the KAON 99 Conference, Chicago, 1999
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KTeV Collaboration, presented by Y. B. Hsiung at the KAON 99 Conference, Chicago, 1999.
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