Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
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Large linear magnetoresistance in a GaAs/AlGaAs heterostructure<br />
Mohammed Ali Aamir, 1 Srijit Goswami, 1 Matthias Baenninger, 2 Vikram<br />
Tripathi, 3 Michael Pepper, 4 Ian Farrer, 2 David A. Ritchie, 2 and Arindam Ghosh 1<br />
1 Department <strong>of</strong> <strong>Physics</strong>, Indian Institute <strong>of</strong> Science, Bangalore 560 012, India.<br />
2 Cavendish Laboratory, University <strong>of</strong> Cambridge,<br />
J.J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom.<br />
3 Department <strong>of</strong> Theoretical <strong>Physics</strong>, Tata Institute <strong>of</strong> Fundamental Research, Homi Bhabha Road, Mumbai 400005, India<br />
4 Department <strong>of</strong> Electrical and Electronic Engineering,<br />
University College, London WC1E 7JE, United Kingdom<br />
Large electrical response to magnetic field is one <strong>of</strong> the key requirements in materials engineering<br />
today. It may seem that a magnetic nature <strong>of</strong> the material is vital for this [1], but some materials<br />
exhibit it even without magnetism at any scale. Over the last decade, it has been shown that<br />
material inhomogeneity alone can provide a route to large magnetoresistance (MR) in non-magnetic<br />
semiconductors [2, 3]. Interestingly, this MR also has a linear characteristic. Here, we study the MR<br />
<strong>of</strong> a two-dimensional electron system (2DES) in a GaAs/AlGaAs heterostructure where a disordered<br />
band-structure is induced by applying a large negative gate bias. We find that MR increases linearly<br />
with magnetic field when the device is operated in the non-equilibrium regime with high sourcedrain<br />
bias [4]. Remarkably, the magnitude <strong>of</strong> MR is as large as 500% per Tesla, thus dwarfing most<br />
non-magnetic materials which exhibit this linearity. Its primary advantage over other materials is<br />
that both linearity and the enormous magnitude are retained over a broad temperature range (0.3 K<br />
to 10 K), thus making it an attractive candidate for on-chip magnetic field sensing.<br />
[1] M. N. Baibich, J. M. Broto, A. Fert, F. N. Van Dau, F. Petr<strong>of</strong>f, P. Etienne, G. Creuzet, A. Friederich, and J. Chazelas,<br />
Phys. Rev. Lett. 61, 2472 (1988).<br />
[2] R. Xu, A. Husmann, T. F. Rosenbaum, M. Saboungi, J. E. Enderby, and P. B. Littlewood, Nature 390, 57 (1997).<br />
[3] M. P. Delmo, S. Yamamoto, S. Kasai, T. Ono, and K. Kobayashi, Nature 457, 1112 (2009).<br />
[4] M. A. Aamir, S. Goswami, M. Baenninger, V. Tripathi, M. Pepper, I. Farrer, D. A. Ritchie, and A. Ghosh, Phys. Rev. B<br />
86, 081203 (2012),