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Thermal Mechanism of Absolute Negative Conductivity in Two-Dimensional Electron Systems
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APS/123-QED
Thermal Mechanism of Absolute Negative Conductivity
in Two-Dimensional Electron Systems
V. Ryzhii?
Computer Solid State Physics Laboratory, University of Aizu, Aizu-Wakamatsu 965-8580, Japan
(Dated: February 2, 2008)
We calculate the dissipative dc conductivity of a two-dimensional electron system in a magnetic
field for the situation when its effective temperature exceeds the temperature of the acoustic phonon
system. We demonstrate that at sufficiently large difference between the electron and lattice temper-
atures (sufficiently strong microwave radiation) the dissipative dc conductivity can become negative.
As an illustration, the case of the electron heating by microwave radiation is considered.
PACS numbers: PACS numbers: 73.40.-c, 78.67.-n, 73.43.-f
I. INTRODUCTION
Recent experimental studies of new types of magne-
toresistance oscillations in a two-dimensional electron
system (2DES) in a magnetic field [1, 2, 3, 4, 5], partic-
ularly the observation of vanishing electrical resistance
caused by microwave radiation, have stimulated exten-
sive efforts to clarify the origin of the uncovered phe-
nomena. The occurrence of the effect of the so-called
zero-resistance states is closely associated with the effect
of absolute negative conductivity (ANC) when the dissi-
pative dc conductivity σ is negative [6, 7, 8]. Mechanisms
of ANC in a 2DES subjected to a magnetic field un-
der nonequilibrium conditions, in particular under irra-
diation with microwaves, have been studied theoretically
since the late 60s [9, 10, 11, 12, 13, 14, 15, 16, 17]. One
can speculate that the photon-assisted impurity scatter-
ing [11, 12, 13] is the main mechanism of ANC causing
the zero-resistance states. Notwithstanding this, a revi-
sion of alternate possible mechanisms of ANC may be of
interest as well.
In this paper, we show that ANC can occur owing to
the electro
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