2014
DOI: 10.1103/physrevlett.113.043001
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Correction of Arbitrary Field Errors in Population Inversion of Quantum Systems by Universal Composite Pulses

Abstract: We introduce universal broadband composite pulse sequences for robust high-fidelity population inversion in two-state quantum systems, which compensate deviations in any parameter of the driving field (e.g., pulse amplitude, pulse duration, detuning from resonance, Stark shifts, unwanted frequency chirp, etc.) and are applicable with any pulse shape. We demonstrate the efficiency and universality of these composite pulses by experimental data on rephasing of atomic coherences in a Pr(3+):Y(2)SiO(5) crystal.

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Cited by 129 publications
(155 citation statements)
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“…Hence, with regard to the diagonal elements U kk , the DR sequence for qutrits (13) is The rephasing error (infidelity) is defined as the distance between the actual propagator and the desired identity matrix,…”
Section: Effects Of Finite Pulse Durationmentioning
confidence: 99%
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“…Hence, with regard to the diagonal elements U kk , the DR sequence for qutrits (13) is The rephasing error (infidelity) is defined as the distance between the actual propagator and the desired identity matrix,…”
Section: Effects Of Finite Pulse Durationmentioning
confidence: 99%
“…,N) can be rephased in a similar manner as the two-, three-, and four-state systems above with a set of free-evolution intervals sandwiched by π pulses applied on the transition between two of the N states at a time. The DR sequences can be built by starting with the sequence π jk τ π jk and then prepend or append π pulses on new pairs of states until all states (for N even) or all states but one (for N odd) (13) in Fig. 4(c) vs the rephasing pulse width T .…”
Section: Rephasing Sequences For Quditsmentioning
confidence: 99%
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“…We make no assumptions about Ω(t) and ∆ (p) (t), which may vary for the different qubits. The dynamics of a qubit due to a pulse is described by a propagator U pulse , which connects the density matrices of the system at the initial and final times t ı and t f : ρ(t f ) = U pulse ρ(t ı )U † pulse and can be parametrized [15] as…”
mentioning
confidence: 99%
“…A phase shift φ in the Rabi frequency, Ω(t) → Ω(t)e ıφ , is imprinted in U pulse as β → β + φ [15][16][17]. The phase φ is assumed the same for every qubit (unlike β), which is usually experimentally feasible.…”
mentioning
confidence: 99%