Hauptseite > Publikationsdatenbank > New Limit on the Permanent Electric Dipole Moment of Xe 129 Using He 3 Comagnetometry and SQUID Detection > print |
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024 | 7 | _ | |a 10.1103/PhysRevLett.123.143003 |2 doi |
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024 | 7 | _ | |a 1079-7114 |2 ISSN |
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100 | 1 | _ | |a Sachdeva, N. |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
245 | _ | _ | |a New Limit on the Permanent Electric Dipole Moment of Xe 129 Using He 3 Comagnetometry and SQUID Detection |
260 | _ | _ | |a College Park, Md. |c 2019 |b APS |
336 | 7 | _ | |a article |2 DRIVER |
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336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1711016937_27452 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a ARTICLE |2 BibTeX |
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336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
520 | _ | _ | |a We report results of a new technique to measure the electric dipole moment of 129Xe with 3Hecomagnetometry. Both species are polarized using spin-exchange optical pumping, transferred to ameasurement cell, and transported into a magnetically shielded room, where SQUID magnetometersdetect free precession in applied electric and magnetic elds. The result from a one week measurementcampaign in 2017 and a 2.5 week campaign in 2018, combined with detailed study of systematiceects, is dA(129Xe) = (1:4 6:6stat 2:0syst) 1028 e cm. This corresponds to an upper limit ofjdA(129Xe)j < 1:4 1027 e cm (95% CL), a factor of ve more sensitive than the limit set in 2001. |
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700 | 1 | _ | |a Singh, J. T. |0 P:(DE-HGF)0 |b 18 |
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773 | _ | _ | |a 10.1103/PhysRevLett.123.143003 |g Vol. 123, no. 14, p. 143003 |0 PERI:(DE-600)1472655-5 |n 14 |p 143003 |t Physical review letters |v 123 |y 2019 |x 1079-7114 |
856 | 4 | _ | |u https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.123.143003 |
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