Spin polarization of two-dimensional electrons in GaAs quantum wells around Landau level filling ν=1 from NMR measurements of gallium nuclei -: art. no. 085327

被引:13
作者
Melinte, S [1 ]
Freytag, N
Horvatic, M
Berthier, C
Lévy, LP
Bayot, V
Shayegan, M
机构
[1] Catholic Univ Louvain, Unite PCPM, B-1348 Louvain, Belgium
[2] MPI FKF, Grenoble High Magnet Field Lab, F-38042 Grenoble 9, France
[3] CNRS, F-38042 Grenoble 9, France
[4] Univ Grenoble 1, Spectrometrie Phys Lab, F-38402 St Martin Dheres, France
[5] Inst Univ France, F-38402 St Martin Dheres, France
[6] Catholic Univ Louvain, Unite DICE, B-1348 Louvain, Belgium
[7] Princeton Univ, Dept Elect Engn, Princeton, NJ 08544 USA
关键词
D O I
10.1103/PhysRevB.64.085327
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
A nuclear magnetic resonance (NMR) study has been carried out con a GaAs/Al0.3Ga0.7As multiple-quantum-well sample, containing two-dimensional (2D) electron layers, in the quantum Hall regime. The spin polarization To of 2D electrons is determined from the hyperfine shift of Ga-69,Ga-71 nuclei, measured by standard pulsed NMR. We have used the tilted-magnetic field technique to investigate the effect of an increasing Zeeman energy on To around Landau level filling factor nu =1. Mostly on the basis of measurements performed at B = 17 T and T = 1.5 K, we conjecture that in the high-B and low-T limit, P(nu) follows the predictions of the noninteracting-electron model. The low-temperature P(nu =1) is found to be far below the expected full polarization, and the observed nuclear spin-lattice relaxation rate is not reduced, in contrast to the observations by optically pumped NMR. The two techniques obtain different results only close to nu =1, and the reason why remains unclear; simple explanation in terms of the nonuniform electron density does not seem satisfactory.
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