phenomenon 105.32 The neutron has no measurable electric dipole moment

open in the book · parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2602 · p. 2140

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phenomenon 105.32: The neutron has no measurable electric dipole moment105.32equation 105.92: eq:cpt-edm-sensitivity105.92equation 105.91: eq:cpt-ramsey-shift105.91theorem 105.30: An EDM violates P and T105.30proof : ch:07-discrete-symmetries-cpt@proof-25proofphenomenon 111.19: The neutron has no electric dipole moment111.19equation 105.17: eq:cpt-C-photon105.17equation 105.6: eq:cpt-P-photon105.6equation 105.30: eq:cpt-T-photon105.30proposition 105.45: The induced neutron electric dipole moment105.45proof : ch:07-discrete-symmetries-cpt@proof-24proof

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typedirectionnode provenancewhere
cites Measurement of the Permanent Electric Dipole Moment of the Neutron derived parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2610
cites Improved Experimental Limit on the Electric Dipole Moment of the Neutron derived parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2611
depends_on eq:cpt-edm-sensitivity declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2617
depends_on eq:cpt-ramsey-shift declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2617
depends_on An EDM violates $P$ and $T$ declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2617
proves ch:07-discrete-symmetries-cpt@proof-25 declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2620