2022
DOI: 10.1103/physreva.105.052438
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Analyzing the Rydberg-based optical-metastable-ground architecture for Yb171 nuclear spins

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Cited by 22 publications
(7 citation statements)
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“…ẋ(t) = v(t), v(t) = F (t)/m with F (t) = mω 2 x(t), with random initial position x(0) and velocity v(0) sampled from a Maxwell-Boltzmann distribution, which is an approximation to the full quantum mechanical problem. Calculations are performed assuming realistic experimental parameters for 171 Yb atoms, including a qubit transition wavelength of 578 nm (standing wave period 289 nm), trap frequency of ω/2π = 100 kHz (trap period τ = 10 µs) and a temperature of 5 µK based on current experiments [20,14,21,22]. The average infidelity of each gate, for different gate times T , was obtained by averaging the infidelity 1 − F obtained from the unitary evolution over 2000 classical trajectories.…”
Section: Otw-1 Osw-1 Osw-bb1mentioning
confidence: 99%
“…ẋ(t) = v(t), v(t) = F (t)/m with F (t) = mω 2 x(t), with random initial position x(0) and velocity v(0) sampled from a Maxwell-Boltzmann distribution, which is an approximation to the full quantum mechanical problem. Calculations are performed assuming realistic experimental parameters for 171 Yb atoms, including a qubit transition wavelength of 578 nm (standing wave period 289 nm), trap frequency of ω/2π = 100 kHz (trap period τ = 10 µs) and a temperature of 5 µK based on current experiments [20,14,21,22]. The average infidelity of each gate, for different gate times T , was obtained by averaging the infidelity 1 − F obtained from the unitary evolution over 2000 classical trajectories.…”
Section: Otw-1 Osw-1 Osw-bb1mentioning
confidence: 99%
“…We follow Ref. [27] and use polarization intensity impurity χ for this discussion, where χ = 0 denotes perfect polarization. We discuss the laser polarization impurity of the three sets of laser fields discussed in Sec.…”
Section: B Influence From Laser Polarization Impuritymentioning
confidence: 99%
“…Numerical simulations with feasible parameters show that nuclear spin coherence can be preserved with a fidelity over 0.999. This theory brings opportunities for coherent control of nuclear-spin quantum memories [23][24][25][26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…Here we show local control of optical transitions in a tweezer-array clock [17][18][19] by using rearrangement techniques [20][21][22][23][24][25] on atoms in superposition states to precisely control the position-dependent phase imprinted by light-matter interaction. The scheme 26,27 is experimentally simple and highly robust as it solely relies on the relative stability of the tweezer positions and does not Article https://doi.org/10.1038/s41567-023-02323-w rotation with the same laser as before; the shifted atom now rotates back to |0〉 because of the movement-induced phase shift, whereas the unmoved atom completes its rotation to |1〉.…”
mentioning
confidence: 99%
“…The main principle behind this scheme is a locally controlled change of the relative phase between the atomic dipole oscillation and the phase of the laser while the atom is in a superposition state; in essence, our scheme realizes a locally controlled Ramsey sequence with global driving (Methods). Similar techniques have been used in the context of ion-trap experiments with two ions 26 , but not in a scalable fashion, as is possible with tweezer arrays 27 .…”
mentioning
confidence: 99%