Abstract

Magnetoresistance measurements of an electron gas formed on a solid-hydrogen substrate are reported as a function of surface disorder. High-mobility surfaces display an essentially classical positive ${B}^{2}$ field dependence. Lower-mobility surfaces, however, are characterized by the appearance of a negative magnetoresistance for fields less than \ensuremath{\sim}0.2 T, in good agreement with present weak-localization theories. On extremely disordered surfaces we find large increases in resistivity but a finite residual electron diffusivity $D\ensuremath{\sim}\frac{\ensuremath{\hbar}}{{m}_{\mathrm{el}}}$.

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