2012
DOI: 10.1038/nmat3499
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Quantum control of hybrid nuclear–electronic qubits

Abstract: Pulsed magnetic resonance allows the quantum state of electronic and nuclear spins to be controlled on the timescale of nanoseconds and microseconds respectively. The time required to flip dilute spins is orders of magnitude shorter than their coherence times, leading to several schemes for quantum information processing with spin qubits. Instead, we investigate 'hybrid nuclear-electronic' qubits consisting of near 50:50 superpositions of the electronic and nuclear spin states. Using bismuth-doped silicon, we … Show more

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Cited by 59 publications
(48 citation statements)
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“…A large number of important defects in the solid state possess such mixing, including donors in silicon, [18][19][20] NV centres in diamond, 21 transition metals in II-VI materials 22 and rare-earth dopants in silicates.…”
Section: -13mentioning
confidence: 99%
“…A large number of important defects in the solid state possess such mixing, including donors in silicon, [18][19][20] NV centres in diamond, 21 transition metals in II-VI materials 22 and rare-earth dopants in silicates.…”
Section: -13mentioning
confidence: 99%
“…The dynamical process underlying NMR can be viewed as the manipulation of magnetization vectors (proportional to spin angular momenta) with pulsed magnetic fields in the radio frequency (rf) regime as controls. Quantum control of spin systems has been treated theoretically and experimentally [9][10][11][12][13][14]. More specifically, for coupled two-spin systems the techniques of polarization or coherence transfer have attracted much interest [15][16][17] motivated by the desire of enhancing the signals of a low gyromagnetic ratio nucleus by transferring to it the larger magnetization of a higher gyromagnetic ratio nucleus [18].…”
Section: Introductionmentioning
confidence: 99%
“…This has in particular been investigated for Si:Bi, where, due to the large hyperfine coupling of Bi, the mixing of electron and nuclear spin occurs at relatively large magnetic fields, allowing for conventional X-band EPR. [13][14][15] Conventional EPR however, requires a thermal equilibrium polarization of the spin system, limiting the sensitivity of conventional EPR to about 10 9 spins at X-band frequencies and typical cryogenic temperatures of the order of 5 K, making low-field experiments challenging. However, by using optical and electrical spin-readout schemes, known as optically/electrically detected magnetic resonance (ODMR/EDMR), single electron and nuclear spins can be detected, their spin state determined, [16][17][18] and the toolbox of sophisticated pulse sequences realized in EPR can be adapted to pulsed EDMR and ODMR.…”
Section: Introductionmentioning
confidence: 99%