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We have observed in a low density two-dimensional hole system (2DHS) ofextremely high quality (with hole density p=1.6x10^{10} cm^{-2} and mobility\mu=0.8x10^6 cm^2/Vs) that, as the 2DHS is continuously tilted with respect tothe direction of the magnetic field, the \nu=1/3 fractional quantum Hall effect(FQHE) state is weakened and its magnetoresistivity rises from ~ 0.4kohm/square in the normal orientation to ~ 180 kohm/square at tilt angle \theta\~ 80 degrees. We attribute this phenomenon to the transition of the 2DHS fromthe FQHE liquid state to the pinned Wigner solid state, and argue that itsorigin is the strong coupling of subband Landau levels under the tiltedmagnetic fields

physical review. b, condensed matter and materials physics

Transition from a fractional quantum Hall liquid to an electron solid at Landau level filling<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ν</mml:mi><mml:mo>=</mml:mo><mml:mstyle scriptlevel="1"><mml:mfrac bevelled="false"><mml:mn>1</mml:mn><mml:mn>3</mml:mn></mml:mfrac></mml:mstyle></mml:math>in tilted magnetic fields

Transition from a fractional quantum Hall liquid to an electron solid at Landau level fillingν=13in tilted magnetic fields