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DOI: 10.1209/epl/i2003-00157-x
Europhys. Lett., 61 (4) , pp. 499-505 (2003)
Hot-hole effects in a dilute two-dimensional gas in
R. Leturcq1, D. L'Hôte1, R. Tourbot1, V. Senz2, U. Gennser3, T. Ihn2, K. Ensslin2, G. Dehlinger4 and D. Grützmacher4
1 DSM/Service de Physique de l'Etat Condensé, CEA-Saclay 91191 Gif-sur-Yvette Cedex, France
2 Laboratory of Solid State Physics, ETH Zürich - CH-8093 Zürich, Switzerland
3 Laboratoire de Photonique et de Nanostructures, CNRS - 91460 Marcoussis, France
4 Paul Scherrer Institut - CH-5232 Villigen PSI, Switzerland
(Received 5 July 2002; accepted in final form 10 December 2002)
Abstract
We study the resistivity vs. electric-field dependence
of a dilute two-dimensional hole (h) system in
, on both sides of the crossover from weak to strong
localization at
B=0. Using
as a "thermometer" to
obtain the effective temperature of the holes
, we
find that
can be attributed to hole heating. In spite
of the strong localization and h-h interactions, the power loss
does not indicate any deviation from the density and temperature
dependences predicted assuming independent and delocalized
electrons. The consequences of these results on the h-h
interaction assisted hopping, glassy behaviour and
E-field
scaling are developed. The hole-phonon coupling involves a
limited screening, a deformation potential compatible with
measurements at larger densities and temperatures, and a
piezoelectric component which is definitely probed.
63.20.Kr - Phonon-electron and phonon-phonon interactions.
73.20.Fz - Weak or Anderson localization.
71.27.+a - Strongly correlated electron systems; heavy fermions.
© EDP Sciences 2003
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