Journal
PHYSICAL REVIEW LETTERS
Volume 87, Issue 8, Pages -Publisher
AMERICAN PHYSICAL SOC
DOI: 10.1103/PhysRevLett.87.086801
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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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