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Kawano, Y.7
Komiyama, S.8
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See also, Y. Kawaguchi, K. Hirakawa, M. Saeki, K. Yamanaka, and S. Komiyama, Appl. Phys. Lett. 80, 136 (2002); B. A. Andreev, I. V. Erofeeva, V. I. Gavrilenko, A. L. Korotkov, A. N. Yablonskiy, O. Astafiev, Y. Kawano, and S. Komiyama, Semicond. Sci. Technol. 16, 300 (2001); N. G. Kalugin, G. Nachtwei, Yu. B. Vasilyev, S. D. Suchalkin, and K. Eberl, Appl. Phys. Lett. 81, 382 (2002).
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11
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20244364807
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note
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Under zero or almost zero current, the capacitance C depends on whether the bulk states in the 2DEG are in localized states or not. It follows that C varies with a sweep of B. However, as in the present measurement, when the sensor is placed in the conductive edge region of the sample and the current densities are relatively high (0.2 A/m for the sensor and 0.13 A/m for the sample), C can be regarded as being approximately constant.
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13
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0346707270
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A. J. Kil, R. J. J. Zijlstra, P. M. Koenraad, J. A. Pals, and J. P. Andre, Solid State Commun. 60, 831 (1986); A. J. Kil, R. J. J. Zijlstra, M. F. H. Schuurmans, and J. P. Andre, Phys. Rev. B 41, 5169 (1990).
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Solid State Commun.
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Kil, A.J.1
Zijlstra, R.J.J.2
Koenraad, P.M.3
Pals, J.A.4
Andre, J.P.5
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14
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0038856573
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A. J. Kil, R. J. J. Zijlstra, P. M. Koenraad, J. A. Pals, and J. P. Andre, Solid State Commun. 60, 831 (1986); A. J. Kil, R. J. J. Zijlstra, M. F. H. Schuurmans, and J. P. Andre, Phys. Rev. B 41, 5169 (1990).
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Phys. Rev. B
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Kil, A.J.1
Zijlstra, R.J.J.2
Schuurmans, M.F.H.3
Andre, J.P.4
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15
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20244386535
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note
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In general, as the channel size is reduced (typically below 0.5 μm), the condition is no longer exactly quantized. However, exact quantization does not matter for an application as an electrometer. As shown in Fig. 2, oscillation of longitudinal resistance with a sweep of B is the essential feature.
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