(109) and the Hamiltonian is given by ˜H(t) = g0        0 e− iω − t e− iω +t eiω − t 0 0 eiω +t 0 0       

In the three-dimensional manifold, the state vector is expressed as |ψ (t)⟩ =c0(t) |0, 0⟩ +c+ 1 (t) |1, 2iη⟩ +c− 1 (t) |1, − 2iη⟩

1 Pith paper cite this work. Polarity classification is still indexing.

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High-Fidelity Raman Spin-Dependent Kicks in the Presence of Micromotion

quant-ph · 2025-11-20 · unverdicted · novelty 6.0

A scheme using modulated Raman pulses achieves spin-dependent kick infidelities below 10^{-5} in trapped ions despite micromotion by optimizing RF parameters to cancel backward kicks.

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High-Fidelity Raman Spin-Dependent Kicks in the Presence of Micromotion quant-ph · 2025-11-20 · unverdicted · none · ref 71
A scheme using modulated Raman pulses achieves spin-dependent kick infidelities below 10^{-5} in trapped ions despite micromotion by optimizing RF parameters to cancel backward kicks.

(109) and the Hamiltonian is given by ˜H(t) = g0        0 e− iω − t e− iω +t eiω − t 0 0 eiω +t 0 0       

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