{ "id": "cond-mat/9903165", "version": "v1", "published": "1999-03-10T12:41:55.000Z", "updated": "1999-03-10T12:41:55.000Z", "title": "Raman scattering in a two-dimensional electron gas: Boltzmann equation approach", "authors": [ "E. G. Mishchenko" ], "comment": "4 pages, 3 figures. to appear in Phys. Rev. B 59 (1999)", "journal": "Phys. Rev. B 59, 14892 (1999).", "doi": "10.1103/PhysRevB.59.14892", "categories": [ "cond-mat.mes-hall", "cond-mat.mtrl-sci" ], "abstract": "The inelastic light scattering in a 2-d electron gas is studied theoretically using the Boltzmann equation techniques. Electron-hole excitations produce the Raman spectrum essentially different from the one predicted for the 3-d case. In the clean limit it has the form of a strong non-symmetric resonance due to the square root singularity at the electron-hole frequency $\\omega = vk$ while in the opposite dirty limit the usual Lorentzian shape of the cross section is reestablished. The effects of electromagnetic field are considered self-consistently and the contribution from collective plasmon modes is found. It is shown that unlike 3-d metals where plasmon excitations are unobservable (because of very large required transfered frequencies), the two-dimensional electron system gives rise to a low-frequency ($\\omega \\propto k^{1/2}$) plasmon peak. A measurement of the width of this peak can provide data on the magnitude of the electron scattering rate.", "revisions": [ { "version": "v1", "updated": "1999-03-10T12:41:55.000Z" } ], "analyses": { "keywords": [ "two-dimensional electron gas", "boltzmann equation approach", "raman scattering", "boltzmann equation techniques", "electron-hole excitations produce" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. B" }, "note": { "typesetting": "TeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable" } } }