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Using Molecules to Measure Nuclear Spin-Dependent Parity Violation
Open accessAbstract
Nuclear spin-dependent parity violation arises from weak interactions between electrons and nucleons and from nuclear anapole moments. We outline a method to measure such effects, using a Stark-interference technique to determine the mixing between opposite-parity rotational/hyperfine levels of ground-state molecules. The technique is applicable to nuclei over a wide range of atomic number, in diatomic species that are theoretically tractable for interpretation. This should provide data on anapole moments of many nuclei and on previously unmeasured neutral weak couplings.
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Citations
Cites
Weak neutral currents in atomic physics
Bouchiat, M. A., & Bouchiat, C. C. (1974) · Physics Letters B · doi:10.1016/0370-2693(74)90656-x · Cited by 385
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Kozyryev, I., Baum, L., Matsuda, K., Augenbraun, B. L., Anderegg, L., Sedlack, A. P., & Doyle, J. M. (2017) · Physical Review Letters · doi:10.1103/physrevlett.118.173201 · Cited by 258
Cavity QED in a molecular ion trap
Schuster, D. I., Bishop, L. S., Chuang, I. L., DeMille, D., & Schoelkopf, R. J. (2011) · Physical Review A · doi:10.1103/physreva.83.012311 · Cited by 61
Self-citationThe Search for Parity Violation in Chiral Molecules
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Metadata
- Authors
- DeMille, D., Cahn, S. B., Murphree, D., Rahmlow, D. A., & Kozlov, M. G.
- Venue
- Physical Review Letters
- Publisher
- American Physical Society (APS)
- Published
- 2008-01-17
- Volume
- 100
- Issue
- 2
- Pages
- 023003-023003
- ISSN
- 0031-9007 (ISSN-L)
- 1079-7114
- OpenAlex
- W2000804402
- Cited by
- 210
- References
- 1
- FWCI
- 7.93
- Type
- journal article
- Language
- en
- Open access
- green
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- DeMille, D., Cahn, S. B., Murphree, D., Rahmlow, D. A., & Kozlov, M. G. (2008). Using Molecules to Measure Nuclear Spin-Dependent Parity Violation. Physical Review Letters. https://doi.org/10.1103/physrevlett.100.023003
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Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).
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