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

Physics – Condensed Matter – Strongly Correlated Electrons

Scientific paper

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4 pages, postscript figures included. Revised version

Scientific paper

10.1103/PhysRevLett.87.086801

The 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.

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