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One-dimensional ballistic transport in AlGaAs/GaAs electron waveguides

J. Vac. Sci. Technol. B Volume 7, Issue 6, pp. 2039-2043 (November 1989)

Issue Date: November 1989
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PACS

  • 73.20.Dx
    Electronic structure and electrical properties of surfaces, interfaces, and thin films Surface and interface electron states Electron states in low-dimensional structures (including quantum wells, superlattices, layer structures, and intercalation compounds)
  • 73.40.Kp
    Electronic structure and electrical properties of surfaces, interfaces, and thin films Electronic transport in interface structures IIIV semiconductor-to-semiconductor contacts, (pn) junctions, and heterojunctions
  • YEAR: 1988-89

PUBLICATION DATA

ISSN:
1071-1023 (print)   1520-8567 (online)
Publisher:
AIP is a member of CrossRef AVS
R. E. Behringer, P. M. Mankiewich, G. Timp, R. E. Howard, H. U. Baranger, J. Cunningham, and S. Sampere
AT&T Bell Laboratories, Holmdel, New Jersey 07733
Recently, there has been growing interest in exploring the limits to scaling of semiconductor devices, and in understanding their characteristics in the regime where quantum effects and ballistic transport dominate. Using high-resolution fabrication techniques on high-mobility, modulation-doped AlGaAs/GaAs, it is possible to confine the two-dimensional electron gas (2DEG) to structures that are smaller than both the inelastic and elastic scattering lengths, and are comparable in size to the electron wavelength. The conduction of such a device should be one dimensional and ballistic. Unlike large samples, the resistance of these ballistic devices does not follow classical equations; it is primarily caused by electron interference and scattering from the geometry of the sample, not by impurities. On this scale, these structures behave as electron waveguides not as diffusive conductors. We have used electron-beam lithography and high-resolution reaction ion etching to produce samples with well controlled, complicated geometries. These devices use either depletion from an etched surface, or the application of a gate voltage to electrostatically confine the 2DEG to a narrow conducting channel. Transport measurements exhibit electron interference effects, nonlocal resistance fluctuations, resistance that does not scale with length, and quantization-of-resistance as a function of width and carrier density. The experiments correspond well to theoretical calculations of simple electron waveguides, and show that in these one-dimensional ballistic devices, the measured resistance is primarily caused by scattering from the structure of the sample itself.
History: Received 19 June 1989; accepted 19 July 1989
Permalink: http://dx.doi.org/10.1116/1.584644

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