论文标题
平面门内诱导基于INAS的量子井中自旋分辨Landau水平的过渡不对称性
In-plane gate induced transition asymmetry of spin-resolved Landau levels in InAs-based quantum wells
论文作者
论文摘要
从横向电场和垂直磁场的跨二维电子传输到准二维电子传输的跨界进行了交叉,在扩散到Quasiballistic和零场中,对量子霍尔制度进行了研究。平面门和霍尔栏是用Ingaas/Inalas/Inas Quantum制造的,托管2DEG,其载体密度约为6.8 $ \ times $ 10 $^{11} $ CM $ $^{ - 2} $,Mobility,Mobility,Mobility,1.8 $ \ times $ \ times $ 10 $^5 $ CM $^2 $^2 $/vs $ ______________ES均为0.042 $ 0.042。温度下降到50 mk的磁转运测量值,最高12吨的磁力率产生了高效的Landé因子| g $^*$ | = 16, enabling the resolution of spin-split subbands at magnetic fields of 2.5 T. In the quantum Hall regime, electrostatic control of an effective constriction width enables steering of the reflection and transmission of edge channels, allowing a separation of fully spin-polarized edge channels at filling factors $ν$ = 1 und $ν$ = 2. A change in the orientation of a transverse in-plane electric field in the constriction shifts the Zeeman-Split量子霍尔高原之间的过渡比$δ$ b $ \ \ $ 0.1 t,与b $ _ {eff} $ $ \ $ 0.13 T的有效磁场一致,大约$ 0.13 t,这表明状态旋转密度的变化。
The cross-over from quasi-two- to quasi-one-dimensional electron transport subject to transverse electric fields and perpendicular magnetic fields are studied in the diffusive to quasiballistic and zero-field to quantum Hall regime. In-plane gates and Hall-bars have been fabricated from an InGaAs/InAlAs/InAs quantum well hosting a 2DEG with carrier density of about 6.8$\times$10$^{11}$ cm$^{-2}$, mobility of 1.8$\times$10$^5$ cm$^2$/Vs and an effective mass of 0.042$m_e$ after illumination. Magnetotransport measurements at temperatures down to 50 mK and fields up to 12 T yield a high effective Landé-factor of |g$^*$| = 16, enabling the resolution of spin-split subbands at magnetic fields of 2.5 T. In the quantum Hall regime, electrostatic control of an effective constriction width enables steering of the reflection and transmission of edge channels, allowing a separation of fully spin-polarized edge channels at filling factors $ν$ = 1 und $ν$ = 2. A change in the orientation of a transverse in-plane electric field in the constriction shifts the transition between Zeeman-split quantum Hall plateaus by $Δ$B $\approx$ 0.1 T and is consistent with an effective magnetic field of B$_{eff}$ $\approx$ 0.13 T by spin-dependent backscattering, indicating a change in the spin-split density of states.