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- W4386476343 abstract "The Stark-interference technique is commonly used to amplify the feeble parity-violating signal in atomic experiments. As a result, interpretation of these experiments in terms of electroweak observables requires knowledge of the Stark-induced $E1$ transition amplitudes or, equivalently, transition polarizabilities. While the literature assumes that these transition polarizabilities do not depend on the nuclear spin, here we prove the contrary. The nuclear-spin dependence arises due to the hyperfine mixing of atomic states and requires a third-order perturbation theory (one hyperfine interaction and two electric-dipole interactions) treatment. We demonstrate that the so far neglected tensor contribution appears in the transition polarizability and present numerical results for the nuclear-spin-dependent corrections to the $6{S}_{1/2}ensuremath{rightarrow}7{S}_{1/2}$ transition polarizability in $^{133}mathrm{Cs}$. We investigate the effect of these corrections to transition polarizabilities on the extraction of the $^{133}mathrm{Cs}$ anapole moment from the Boulder experiment [Science 275, 1759 (1997)]. We also consider their effect on the extraction of the ratio between the scalar and vector transition polarizabilities from the measurements [Phys. Rev. A 55, 1007 (1997)]. While the corrections are minor at the current level of experimental accuracy, our analysis provides a framework for future experiments." @default.
- W4386476343 created "2023-09-07" @default.
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- W4386476343 date "2023-09-06" @default.
- W4386476343 modified "2023-10-11" @default.
- W4386476343 title "Nuclear-spin-dependent corrections to the transition polarizability in cesium" @default.
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- W4386476343 doi "https://doi.org/10.1103/physreva.108.032805" @default.
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