Abstract
We have performed RF experiments on a lateral quantum dot defined in the two dimensional electron gas (2DEG) of a GaAs/AlGaAs heterostructure. The small capacitance of the quantum dot gives rise to single-electron charging effects, which we employed to realize a quantum dot turnstile device. By modulating the tunnel barriers between the quantum dot and the 2DEG leads with two phase-shifted RF signals, we pass an integer number of electrons through the quantum dot per RF cycle. This is demonstrated by the observation of quantized current plateaus at multiples ofef in current-voltage characteristics, wheref is the frequency of the RF signals. When an asymmetry is induced by applying unequal RF voltages, our quantum dot turnstile operates as a single-electron pump producing a quantized current at zero bias voltage.
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See for a review; Averin, D.V., Likharev, K.K.: In: Quantum effects in small disordered systems. Al'tshuler, B., Lee, P., Webb, R. (eds.), Amsterdam Elsevier 1990
See for a recent review, including various semiconductor systems: Grabert, H., Devoret, M.H. (eds.): Proceedings of the NATO ASI onSingle Charge Tunneling, Les Houches, March 1991. New York: Plenum Press 1992
Delsing, P., Likharev, K.K., Kuzmin, L.S., Claeson, T.: Phys. Rev. Lett.63, 1861 (1989); Ref. 2 See for a recent review, including various semiconductor systems: Grabert, H., Devoret, M.H. (eds.): Proceedings of the NATO ASI onSingle Charge Tunneling, Les Houches, March 1991. New York: Plenum Press 1992
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The interplay between charging effects and discrete energy states are reported by: McEuen, P.L., Foxman, E.B., Meirav, U., Kastner, M.A. Meir, Y., Wingreen, N.S., Wind, S.J.: Phys. Rev. Lett.66, 1926 (1991)
Charging experiments on this structure without applying RF signals are reported by: Kouwenhoven, L.P., Vaart, N.C. van der, Johnson, A.T., Kool, W., Harmans, C.J.P.M., Williamson, J.G., Staring, A.A.M.: Z Phys. B—Condensed Matter85, 367 (1991); Kouwenhoven, L.P., Vaart, N.C. van der, Johnson, A.T., Harmans, C.J.P.M., Williamson, J.G., Staring, A.A.M.: In: Festkörperprobleme/Advances in Solid State Physics. Rössler, U. (ed.), Vol. 31, pp. 329–340. Braunschweig: Vieweg 1991
The device described in this paper is different from the device in Ref. 14, Charging experiments on this structure without applying RF signals are reported by: but has the same gate geometry
We neglect the energy separation between the dot's discrete levels, which in this sample is less then a tenth of the charging energy; see also Ref. 14,
Kouwenhoven, L.P., Wees, B.J. van, Harmans, C.J.P.M., Williamson, J.G., Houten, H. van, Beenakker, C.W.J., Foxon, C.T., Harris, J.J.: Phys. Rev. B39, 8040 (1989)
We also found a current plateau atef in a previous sample, but due to intrinsic sample instabilities these results were less clear
Averin, D.V., Nazarov, Yu.V.: Phys. Rev. Lett.65, 2446 (1990)
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Kouwenhoven, L.P., Johnson, A.T., van der Vaart, N.C. et al. Quantized current in a quantum dot turnstile. Z. Physik B - Condensed Matter 85, 381–388 (1991). https://doi.org/10.1007/BF01307634
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DOI: https://doi.org/10.1007/BF01307634