We report the influence of voltmeters on measurements of the longitudinal resistance Rxx in the quantum Hall-effect regime. We show that for input resistances typical of standard digital lock-in amplifiers, Rxx can show a nonzero minimum which might be mistaken for a parallel conduction in the doping layer. This residual impedance at the Rxx minima can be calculated with Zres = R xy 2 Rin +jωC R xy 2, where Rin is the input resistance of the voltmeter, C is the measurement capacitance, and Rxy=h/νe2 is the Hall resistance. In contrast to a real parallel conduction, the effect disappears when either the current source and ground contact are swapped or the polarity of the magnetic field is changed; examples with data are shown. We discuss how proper phasing of a lock-in amplifier is necessary to eliminate false residual minima which arise from stray capacitances.
|Original language||English (US)|
|Journal||Journal of Applied Physics|
|State||Published - Jul 1 2005|
ASJC Scopus subject areas
- Physics and Astronomy(all)