2010
DOI: 10.1103/physrevd.82.076001
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Improved constraints on isotropic shift and anisotropies of the speed of light using rotating cryogenic sapphire oscillators

Abstract: We demonstrate that Michelson-Morley tests, which detect direction-dependent anisotropies in the speed of light, can also be used to place limits upon isotropic deviations of the vacuum speed of light from c, as described by the photon-sector standard model extension parameter tr . A shift in the speed of light that is isotropic in one inertial frame implies anisotropic shifts in others. Using observer Lorentz covariance, we derive the time-dependent variations in the relative resonance frequencies of a pair o… Show more

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Cited by 36 publications
(38 citation statements)
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“…The value forκ tr determined from this experiment isκ tr = 3.4 ± 6.2 × 10 −9 (1σ error), the tightest published constraint onκ tr to our knowledge. This constraint is more than a factor of 12 better than previous test of LI at optical frequencies [13] and moderately better than the previous best [9]. This exper- iment is the first odd-parity optical resonator experiment and the use of counter propagating modes enables a new constraint onκ tr using a non-rotating resonator without temperature control, vibration isolation or vacuum systems.…”
Section: Discussionmentioning
confidence: 75%
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“…The value forκ tr determined from this experiment isκ tr = 3.4 ± 6.2 × 10 −9 (1σ error), the tightest published constraint onκ tr to our knowledge. This constraint is more than a factor of 12 better than previous test of LI at optical frequencies [13] and moderately better than the previous best [9]. This exper- iment is the first odd-parity optical resonator experiment and the use of counter propagating modes enables a new constraint onκ tr using a non-rotating resonator without temperature control, vibration isolation or vacuum systems.…”
Section: Discussionmentioning
confidence: 75%
“…For the scalar parameterκ tr the result is 3.4 ± 6.2 × 10 −9 , a new limit on the constraint. The uncompetitive constraint placed on the odd parameterκ XZ o+ compared to the scalar parameterκ tr is because the current best constraints are derived from experiments with different sensitivities ( [7,8] and [9] respectively) and in this first realization of an asymmetric optical resonator we use a non-rotating experiment, giving reduced sensitivity to the odd parameters [10].…”
Section: Discussionmentioning
confidence: 99%
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“…•Photon Tests [112,113,114,115,116,117,118,119,120,121,122,123,124]: The relevant leading-order terms for the photon sector in the SME are the k AF and k F terms in Eq. (23).…”
Section: Examplesmentioning
confidence: 99%
“…[10], the same authors classified the components of the rank-4 tensor (K F ) µναβ into birefringent and nonbirefrintent. Since those works, this CP T -even, but Lorentz-violating, parametrization has been the subject of diverse works in both the theoretical [20,[22][23][24][25][26][27][28][29][30][31][32] and experimental [33][34][35][36] sides. There is a clear difference concerning the experimental sensitivity reached for each set of parameters, for the constraints established for the birefringent coefficients are more stringent than the current bounds restricting the nonbirefringent components by several orders of magnitude.…”
Section: The Nonbirefringent Lorentz-violating Photon Propagatormentioning
confidence: 99%