Magneto-Optical Properties of Wurtzite-Phase InP Nanowires

被引:21
作者
De Luca, M. [1 ,2 ]
Polimeni, A. [1 ,2 ]
Fonseka, H. A. [3 ]
Meaney, A. J. [4 ]
Christianen, P. C. M. [4 ]
Maan, J. C. [4 ]
Paiman, S. [3 ]
Tan, H. H. [3 ]
Mura, F. [5 ]
Jagadish, C. [3 ]
Capizzi, M. [1 ,2 ]
机构
[1] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[2] Univ Roma La Sapienza, CNISM, I-00185 Rome, Italy
[3] Australian Natl Univ, Dept Elect Mat Engn, Res Sch Phys & Engn, Canberra, ACT 0200, Australia
[4] Radboud Univ Nijmegen, Inst Mol & Mat, High Field Magnet Lab, NL-6525 ED Nijmegen, Netherlands
[5] Univ Roma La Sapienza, Dipartimento Sci Base & Applicate Ingn, I-00185 Rome, Italy
基金
澳大利亚研究理事会;
关键词
Semiconductor nanowires; wurtzite-phase InP; magneto-photoluminescence; effective mass; gyromagnetic factor; DEPENDENT PHOTOLUMINESCENCE; OPTICAL-PROPERTIES; BAND; TEMPERATURE; EXCITON; MAGNETOREFLECTANCE; ZINCBLENDE; CDS;
D O I
10.1021/nl500870e
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The possibility to grow in zincblende (ZB) and/or wurtzite (WZ) crystal phase widens the potential applications of semiconductor nanowires (NWs). This is particularly true in technologically relevant III-V compounds, such as GaAs, In As, and InP, for which WZ is not available in bulk form. The WZ band structure of many III-V NWs has been widely studied. Yet, transport (that is, carrier effective mass) and spin (that is, carrier g-factor) properties are almost experimentally unknown. We address these issues in a well-characterized material: WZ indium phosphide. The value and anisotropy of the reduced mass (mu(exc)) and g-factor (g(exc)) of the band gap exciton are determined by photoluminescence measurements under intense magnetic fields (B, up to 28 T) applied along different crystallographic directions. mu(exc) is 14% greater in WZ NWs than in a ZB bulk reference and it is 6% greater in a plane containing the WZ (c) over cap axis than in a plane orthogonal to (c) over cap. The Zeeman splitting is markedly anisotropic with g(exc) = vertical bar g(e)vertical bar = 1.4 for B perpendicular to(c) over cap (where g(e) is the electron g-factor) and g(exc) = vertical bar g(e) - g(h,/) (/)vertical bar = 3.5 for B/ /(c) over cap (where g(h,/ /) is the hole g-factor). A noticeable B-induced circular dichroism of the emitted photons is found only for B/ /(c) over cap, as expected in WZ-phase materials.
引用
收藏
页码:4250 / 4256
页数:7
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