Magneto-optical properties of wurtzite-phase InP nanowires
Nano letters, 2014•ACS Publications
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, InAs, 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 …
potential applications of semiconductor nanowires (NWs). This is particularly true in
technologically relevant III–V compounds, such as GaAs, InAs, 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 …
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, InAs, 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 (μexc) and g-factor (gexc) of the band gap exciton are determined by photoluminescence measurements under intense magnetic fields (B, up to 28 T) applied along different crystallographic directions. μexc is 14% greater in WZ NWs than in a ZB bulk reference and it is 6% greater in a plane containing the WZ ĉ axis than in a plane orthogonal to ĉ. The Zeeman splitting is markedly anisotropic with gexc = |ge| = 1.4 for B⊥ĉ (where ge is the electron g-factor) and gexc = |ge – gh,//| = 3.5 for B//ĉ (where gh,// is the hole g-factor). A noticeable B-induced circular dichroism of the emitted photons is found only for B//ĉ, as expected in WZ-phase materials.
ACS Publications
以上显示的是最相近的搜索结果。 查看全部搜索结果