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Bulletin of the American Physical Society

Evidence for Nuclear Magnetic Octupole Moments in 133Cs and 87Rb from Measurements of Hyperfine Intervals

Carol E. Tanner, Vladislav P. Gerginov, W. R. Johnson

Published May 23, 2009• 0 citations
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Magnetic resonance in quantum computing and in accurate measurements of the nuclear moments of atoms and molecules

Zhichen Liu, Richard A. Klemm

Modern experimental techniques can generate magnetic fields of the form H(t) = H0 z-hat + H1 [x-hat cos(ωt) + y-hat sin(ωt)], at frequencies within an order of magnitude of the nuclear magnetic resonance (NMR) and electron paramagnetic resonance (EPR) frequencies, ωn0 and ωe0, respectively, when acting on atoms or molecules. We derive simple closed-form expressions for the exact nuclear- and electronic-spin wave functions that enable controlled transitions between entangled states, allowing an atom or molecule to function as a quantum computer. These solutions also enable precise NMR or EPR measurements of nuclear moments in atoms and molecules. We present examples relevant to measurements of the nuclear moments of 14N, 7Li, and 133Cs. Because existing hyperfine measurements of the lowest three nuclear moments of 133Cs are mutually inconsistent, the proposed NMR/EPR experiments provide a route to measuring all seven of its nuclear moments with high precision.

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Hyperfine structure determination of the 72D52state of 133Cs

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MEASUREMENT OF SPIN-EXCHANGE CROSS SECTIONS FOR $sup 133$Cs, $sup 87$Rb, $sup 85$Rb, $sup 39$K, AND $sup 23$Na.

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High-Resolution Spectroscopy of $^{173}$Yb$^{+}$ Ions

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Compared to other stable isotopes of $\rm{Yb}^+$, $^{173}\rm{Yb}^+$ has a richer hyperfine structure, which leads to more favorable clock transitions, spectroscopic techniques for probing new physics, and more sophisticated quantum computing architectures. However, to date, its electronic spectrum remains poorly characterized. Here, we report on efficient laser cooling, state preparation, and detection of a single trapped $^{173}\rm{Yb}^+$ ion. The previously unobserved $^2\!S_{1/2} \rightarrow {}^2\!D_{3/2}$ electric quadrupole transition at 436 nm is coherently excited, and the isotope shift between $^{171}\rm{Yb}^+$ and $^{173}\rm{Yb}^+$ on this transition is determined with an uncertainty of 1.4 Hz. Using microwave spectroscopy, we resolve the hyperfine structure (HFS) of the ${}^2\!D_{3/2}$ state with a relative uncertainty below $10^{-8}$. From the HFS measurement data, we infer for ${}^{173}$Yb a nuclear magnetic octupole moment $Ω= -0.062(8)\,({\rm b} \times μ_N)$ with uncertainty reduced by more than 2 orders of magnitude compared to previous studies. The data also allow us to determine hyperfine anomalies for the ${}^2\!S_{1/2}$ and ${}^2\!D_{3/2}$ states.

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Magnetic Trapping of an Ultracold 87 Rb - 133 Cs Atomic Mixture

Patrick Tierney

This thesis reports on the realisation and characterisation of a magnetically trapped ultracold atomic mixture of 87Rb and 133Cs in the F = 1, mF = −1 and F = 3, mF = −3 hyperfine states respectively. A compact two-species double magneto-optical trapping (MOT) apparatus is constructed in which a pyramid MOT acts to provide an independent flux of both atomic species for capture in the ultra-high vacuum science region of the apparatus. For the two-species science MOT in which this atom flux is captured, interspecies light assisted inelastic collisions are found to be a highly significant loss mechanism. A novel optical pressure spatial displacement technique is developed to minimise such losses, allowing near independent simultaneous loading of up to ' 8 × 108 87Rb and ' 3 × 108 133Cs atoms into an Ioffe-Pritchard ‘baseball ’ magnetic trap at magnetic bias fields of 166.70(6) and 165.50(6) G respectively. At the loaded 87Rb and 133Cs atom number densities of 1.78(6) × 109 and

•Jan 1, 2009•1 citation

Hyperfine Constants for Low-Lying States in ^137Ba^+

Yu, Kai-Zhi

理论物理通讯:英文版•Jan 1, 2007•0 citations
Modern experimental techniques can generate magnetic fields of the form H(t) = H0 z-hat + H1 [x-hat cos(ωt) + y-hat sin(ωt)], at frequencies within an order of magnitude of the nuclear magnetic resonance (NMR) and electron paramagnetic resonance (EPR) frequencies, ωn0 and ωe0, respectively, when acting on atoms or molecules. We derive simple closed-form expressions for the exact nuclear- and electronic-spin wave functions that enable controlled transitions between entangled states, allowing an atom or molecule to function as a quantum computer. These solutions also enable precise NMR or EPR measurements of nuclear moments in atoms and molecules. We present examples relevant to measurements of the nuclear moments of 14N, 7Li, and 133Cs. Because existing hyperfine measurements of the lowest three nuclear moments of 133Cs are mutually inconsistent, the proposed NMR/EPR experiments provide a route to measuring all seven of its nuclear moments with high precision.
MEASUREMENT OF SPIN-EXCHANGE CROSS SECTIONS FOR sup133sup 133sup133Cs, sup87sup 87sup87Rb, sup85sup 85sup85Rb, sup39sup 39sup39K, AND sup23sup 23sup23Na.
High-Resolution Spectroscopy of 173^{173}173Yb+^{+}+ Ions
Compared to other stable isotopes of Yb+\rm{Yb}^+Yb+, 173Yb+^{173}\rm{Yb}^+173Yb+ has a richer hyperfine structure, which leads to more favorable clock transitions, spectroscopic techniques for probing new physics, and more sophisticated quantum computing architectures. However, to date, its electronic spectrum remains poorly characterized. Here, we report on efficient laser cooling, state preparation, and detection of a single trapped 173Yb+^{173}\rm{Yb}^+173Yb+ ion. The previously unobserved 2 ⁣S1/2→2 ⁣D3/2^2\!S_{1/2} \rightarrow {}^2\!D_{3/2}2S1/2​→2D3/2​ electric quadrupole transition at 436 nm is coherently excited, and the isotope shift between 171Yb+^{171}\rm{Yb}^+171Yb+ and 173Yb+^{173}\rm{Yb}^+173Yb+ on this transition is determined with an uncertainty of 1.4 Hz. Using microwave spectroscopy, we resolve the hyperfine structure (HFS) of the 2 ⁣D3/2{}^2\!D_{3/2}2D3/2​ state with a relative uncertainty below 10−810^{-8}10−8. From the HFS measurement data, we infer for 173{}^{173}173Yb a nuclear magnetic octupole moment Ω=−0.062(8) (b×μN)Ω= -0.062(8)\,({\rm b} \times μ_N)Ω=−0.062(8)(b×μN​) with uncertainty reduced by more than 2 orders of magnitude compared to previous studies. The data also allow us to determine hyperfine anomalies for the 2 ⁣S1/2{}^2\!S_{1/2}2S1/2​ and 2 ⁣D3/2{}^2\!D_{3/2}2D3/2​ states.
This thesis reports on the realisation and characterisation of a magnetically trapped ultracold atomic mixture of 87Rb and 133Cs in the F = 1, mF = −1 and F = 3, mF = −3 hyperfine states respectively. A compact two-species double magneto-optical trapping (MOT) apparatus is constructed in which a pyramid MOT acts to provide an independent flux of both atomic species for capture in the ultra-high vacuum science region of the apparatus. For the two-species science MOT in which this atom flux is captured, interspecies light assisted inelastic collisions are found to be a highly significant loss mechanism. A novel optical pressure spatial displacement technique is developed to minimise such losses, allowing near independent simultaneous loading of up to ' 8 × 108 87Rb and ' 3 × 108 133Cs atoms into an Ioffe-Pritchard ‘baseball ’ magnetic trap at magnetic bias fields of 166.70(6) and 165.50(6) G respectively. At the loaded 87Rb and 133Cs atom number densities of 1.78(6) × 109 and