Indication of the ferromagnetic instability in a dilute two-dimensional electron system

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dc.creatorShashkin, A. A.
dc.creatorKravchenko, S. V.
dc.creatorDolgopolov, V. T.
dc.creatorKlapwijk, T. M.
dc.date2000-07-25
dc.date2001-05-06
dc.date.accessioned2026-07-07T02:38:18Z
dc.date.available2026-07-07T02:38:18Z
dc.descriptionThe magnetic field B_c, in which the electrons become fully spin-polarized, is found to be proportional to the deviation of the electron density from the zero-field metal-insulator transition in a two-dimensional electron system in silicon. The tendency of B_c to vanish at a finite electron density suggests a ferromagnetic instability in this strongly correlated electron system.
dc.description4 pages, postscript figures included. Revised version
dc.identifierhttps://arxiv.org/abs/cond-mat/0007402
dc.identifierhttp://arxiv.org/abs/cond-mat/0007402
dc.identifierPhys. Rev. Lett. 87, 086801 (2001)
dc.identifierdoi:10.1103/PhysRevLett.87.086801
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/16622
dc.subjectStrongly Correlated Electrons
dc.subjectMesoscale and Nanoscale Physics
dc.titleIndication of the ferromagnetic instability in a dilute two-dimensional electron system
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