{ "id": "cond-mat/9802231", "version": "v2", "published": "1998-02-21T17:13:39.000Z", "updated": "1998-03-04T15:30:46.000Z", "title": "Heating of a two-dimensional electron gas by the electric field of a surface acoustic wave", "authors": [ "I. L. Drichko", "A. M. D'yakonov", "V. D. Kagan", "A. M. Kreshchuk", "T. A. Polyanskaya", "I. G. Savel'ev", "I. Yu. Smirnov", "A. V. Suslov" ], "comment": "some technical corrections for pictures were made", "categories": [ "cond-mat.mes-hall" ], "abstract": "The heating of a two-dimensional electron gas by an rf electric field generated by a surface acoustic wave, which can be described by an electron temperature $T_e$, has been investigated. It is shown that the energy balance of the electron gas is determined by electron scattering by the piezoelectric potential of the acoustic phonons with $T_e$ determined from measurements at frequencies $f$= 30 and 150 MHz. The experimental curves of the energy loss $Q$ versus $T_e$ at different SAW frequencies depend on the value of $\\omega \\bar{\\tau}_{\\epsilon}$, compared to 1, where $ \\bar {\\tau}_{\\epsilon}$ is the relaxation time of the average electron energy. Theoretical calculations of the heating of a two-dimensional electron gas by the electric field of the surface acoustic wave are presented for the case of thermal electrons ($\\Delta T \\ll T$). The calculations show that for the same energy losses $Q$ the degree of heating of the two-dimensional electrons (i.e., the ratio $T_e/T$) for $\\omega \\bar{\\tau}_{\\epsilon}>1$ ($f$= 150 MHz) is less than for $\\omega \\bar{\\tau}_{\\epsilon}<1$ ($f$=30 MHz). Experimental results confirming this calculation are presented.", "revisions": [ { "version": "v2", "updated": "1998-03-04T15:30:46.000Z" } ], "analyses": { "keywords": [ "two-dimensional electron gas", "surface acoustic wave", "saw frequencies depend", "rf electric field", "calculation" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "1998cond.mat..2231D" } } }