1996
DOI: 10.1088/0953-8984/8/25/008
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Electric-field-induced magnetoresistance of lateral superlattices

Abstract: The transverse electric field E y which appears in lateral superlattices (SLs) in the presence of a high applied electric field E x and a low magnetic field H normal to the SL plane (H OZ) is calculated. When the electron energy spectrum is non-additive, the field E y contains both the Hall field and the spontaneous transverse electric field which exists without H. The field E y is a multiple-valued and sign-changing function of E x . The kinetic potential whose minimum corresponds to the stationary state of t… Show more

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Cited by 9 publications
(10 citation statements)
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“…At |H| 1 the current density j, defined by (2.3) and (2.8), may be found analytically in linear approximation on H [13,14]. At high H the calculations cannot be accomplished analytically and some computational problems had to be solved.…”
Section: Sample Configuration and Calculation Of Static Current Densitymentioning
confidence: 99%
“…At |H| 1 the current density j, defined by (2.3) and (2.8), may be found analytically in linear approximation on H [13,14]. At high H the calculations cannot be accomplished analytically and some computational problems had to be solved.…”
Section: Sample Configuration and Calculation Of Static Current Densitymentioning
confidence: 99%
“…At | | 1 H the current density j may be found analytically in the linear approximation on H [1,2]. At high H we use the numerical algorithm described in Section 4.…”
Section: Original Papermentioning
confidence: 99%
“…The influence of a weak magnetic field was investigated in [1,2] and it was shown that even an arbitrary small value of H plays the principal role because it smears out the phase transition and enforces the system to make a completely determinate selection between the conditions that are of equal probability at 0 H = . Thus, forced bifurcation takes place.…”
Section: Original Papermentioning
confidence: 99%
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