2010
DOI: 10.1063/1.3373591
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Electron-nuclear spin control in charged semiconductor quantum dots by electrical currents through micro-coils

Abstract: We have fabricated micrometer-sized single-turn coils on top of charged CdSe/ZnSe quantum dot heterostructures by lithographical techniques. Current injection creates magnetic fields in the some 10 mT range, strong enough to modulate the hyperfine interaction. The very low coil inductance allows for generation of fast field transients. We demonstrate local control of the resident electron spin as well as read-out of the nuclear spin state on the 10 ns time scale by electrical current pulses.

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Cited by 5 publications
(12 citation statements)
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“…Amplitude A versus field B z generated by a superconducting magnet (circles) and versus I coil in both current directions (up and down triangles) . tnormalσ=tnormalσ+=2.5 μs.…”
Section: Resultsmentioning
confidence: 99%
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“…Amplitude A versus field B z generated by a superconducting magnet (circles) and versus I coil in both current directions (up and down triangles) . tnormalσ=tnormalσ+=2.5 μs.…”
Section: Resultsmentioning
confidence: 99%
“…It should be emphasized that the result in Fig. represents the situation for vanishing DNP, because the hyperfine interaction really equalizes the electron spin S and the average nuclear spin J , which in this case is zero due to the equally long pumping intervals tnormalσ and tnormalσ+ and the total cycle duration of only a few µs. In fact, the combination of optical and electrical pulses can be utilized to read‐out the nuclear spin state optically.…”
Section: Resultsmentioning
confidence: 99%
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“…Different experimental methods have been developed to optically or electrically detect the NMR. 15 In this work, we adapt the on-chip microcoil technique to n-GaAs in order to perform NMR measurements on each species of isotopes in GaAs ͑ 69 Ga, 71 Ga, and 75 As͒ and to demonstrate Rabi oscillations of the 75 As nuclear spin ensemble on a spatial scale of below 5 m. Experimentally, an Overhauser field of B N ϳ 35 mT is generated via resonant excitation with circularly polarized light. 9,10 Quite often, the rf field needed for NMR is produced from a Helmholtz coil with a typical power consumption of ϳ100 W or so.…”
mentioning
confidence: 99%