2013
DOI: 10.1103/physreva.87.012512
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Observation of the nuclear magnetic octupole moment of173Yb from precise measurements of the hyperfine structure in the3P2state

Abstract: We measure hyperfine structure in the metastable 3 P 2 state of 173 Yb and extract the nuclear magnetic octupole moment. We populate the state using dipole-allowed transitions through the 3 P 1 and 3 S1 states. We measure frequencies of hyperfine transitions of the 3 P 2 → 3 S1 line at 770 nm using a Rb-stabilized ring cavity resonator with a precision of 200 kHz. Second-order corrections due to perturbations from the nearby 3 P 1 and 1 P 1 states are below 30 kHz. We obtain the hyperfine coefficients as: A = … Show more

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Cited by 20 publications
(33 citation statements)
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“…As can be seen, the CV and CC correlations make significant contributions to these constants. Comparing our results with other recent measurement and calculations by Porsev et al [32] and Singh et al [22], we found an excellent agreement for the A constant. However, this may be an accidental accidental since μ I = −0.648(3) μ N from Ref.…”
Section: B Atomic Structure Calculationssupporting
confidence: 90%
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“…As can be seen, the CV and CC correlations make significant contributions to these constants. Comparing our results with other recent measurement and calculations by Porsev et al [32] and Singh et al [22], we found an excellent agreement for the A constant. However, this may be an accidental accidental since μ I = −0.648(3) μ N from Ref.…”
Section: B Atomic Structure Calculationssupporting
confidence: 90%
“…It was found from Table I that the present B/Q constant differs from theirs by about 9%, which is in better agreement than that from Ref. [22]. For the latter the deviation reaches 14%.…”
Section: B Atomic Structure Calculationssupporting
confidence: 80%
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