Volume 229, Issue 2 pp. 681-684
Original Paper

Spectral Anomalies of Exciton Photoluminescence at ν = 1 and 2/3 in a Modulation-Doped n-Type CdTe/(Cd, Mg, Mn)Te Single Quantum Well

H. Yokoi

H. Yokoi

National Institute of Advanced Industrial Science and Technology, 1-1 Higashi 1-chome, Tsukuba, Ibaraki 305-8565, Japan

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Y. Kakudate

Y. Kakudate

National Institute of Advanced Industrial Science and Technology, 1-1 Higashi 1-chome, Tsukuba, Ibaraki 305-8565, Japan

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S. Fujiwara

S. Fujiwara

National Institute of Advanced Industrial Science and Technology, 1-1 Higashi 1-chome, Tsukuba, Ibaraki 305-8565, Japan

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Y. Kim

Y. Kim

National High Magnetic Field Laboratory, Los Alamos National Laboratory, MS E-536, Los Alamos, NM 87545, USA

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S. Takeyama

S. Takeyama

Faculty of Science, Chiba University, 1-33, Yayoi-cho, Inage-ku, Chiba 263-8522, Japan

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G. Karczewski

G. Karczewski

Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32/46, PL- 02-668 Warsaw, Poland

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T. Wojtowicz

T. Wojtowicz

Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32/46, PL- 02-668 Warsaw, Poland

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J. Kossut

J. Kossut

Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32/46, PL- 02-668 Warsaw, Poland

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Abstract

Spin-polarized magnetophotoluminescence measurements have been conducted in a modulation-doped n-type CdTe/(Cd, Mg, Mn)Te single quantum well at 1.5 K under 2 s long pulsed magnetic fields up to 60 T. For the σ polarization, a new peak was observed to emerge at ν ∼ 1 on the higher energy side of a main peak. The former peak became larger than the latter with increasing magnetic field, while the latter peak had a local maximum at ν ∼ 0.9 and attenuated. Furthermore, magnetic field dependence of the latter peak energy showed step-like behavior around ν ∼ 0.9. The intensity of the former peak was observed to increase monotonically with field, showed a kink at ν ∼ 2/3 and saturated, i.e. showed a shoulder-like structure there. With changing the angle between the direction of the sample surface normal and the magnetic field, both features at ν ∼ 1 and 2/3 exhibited tendencies to fade out, which suggests that the former is associated with spin-singlet charged exciton and the latter with fractional quantum Hall effect at ν = 2/3.

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