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Phys. Rev. Lett. 87, 136801 (2001) [4 pages]

New Phase Transition between Partially and Fully Polarized Quantum Hall States with Charge and Spin Gaps at ν = 2/3

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N. Freytag1,*, Y. Tokunaga1, M. Horvatić1, C. Berthier1,2, M. Shayegan3, and L. P. Lévy1,4
1Grenoble High Magnetic Field Laboratory, MPI-FKF and CNRS, BP 166, F-38042 Grenoble Cedex 9, France
2Laboratoire de Spectrométrie Physique, Université J. Fourier, BP 87, F-38402 St. Martin d'Hères, France
3Department of Electrical Engineering, Princeton University, Princeton, New Jersey 08544
4Institut Universitaire de France and Université J. Fourier, BP 41, F-38402 St. Martin d'Hères, France

Received 30 May 2001; published 7 September 2001

The average electron spin polarization P of a two-dimensional electron gas confined in GaAs/GaAlAs multiple quantum wells was measured by NMR near the fractional quantum Hall state with filling factor ν = 2/3. Above this filling factor ( 2/3ν<0.85), a strong depolarization is observed corresponding to two spin flips per additional flux quantum. The most remarkable behavior of the polarization is observed at ν = 2/3, where a quantum phase transition from a partially polarized ( P3/4) to a fully polarized ( P = 1) state can be driven by increasing the ratio between the Zeeman and the Coulomb energy above a critical value ηc = ΔZ/ΔC = 0.0185.

© 2001 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.87.136801
DOI:
10.1103/PhysRevLett.87.136801
PACS:
73.43.Nq, 71.10.-w, 76.60.Cq

*Corresponding author: freytag@polycnrs-gre.fr