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Magnetointersubband resistance oscillations in GaAs quantum wells placed in a tilted magnetic field

机译:倾斜磁场中的GaAs量子阱中的磁间子带电阻振荡

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摘要

The magnetotransport of highly mobile two-dimensional electrons in wide GaAs single quantum wells with three populated subbands placed in tilted magnetic fields is studied. The bottoms of the lower two subbands have nearly the same energy while the bottom of the third subband has a much higher energy (E_1 ≈ E_2 << E_3). At zero in-plane magnetic fields, magnetointersubband oscillations (MISO) between the ith and jth subbands are observed and obey the relation Δ_(ij) = E_j - E_i = khω_c, where ω_c is the cyclotron frequency and k is an integer. An application of in-plane magnetic field produces dramatic changes in MISO and the corresponding electron spectrum. Three regimes are identified. At hω_c << Δ_(12), the in-plane magnetic field increases considerably the gap Δ_(12), which is consistent with the semiclassical regime of electron propagation. In contrast, at strong magnetic fields hω_c >> Δ_(12) relatively weak oscillating variations of the electron spectrum with the in-plane magnetic field are observed. At hω_c ≈ Δ_(12), the electron spectrum undergoes a transition between these two regimes through magnetic breakdown. In this transition regime MISO with odd quantum number k terminate, while MISO corresponding to even k evolve continuously into the high-field regime corresponding to hω_c >> Δ_(12).
机译:研究了在倾斜磁场中具有三个人口子带的宽GaAs单量子阱中高迁移率二维电子的磁传输。较低的两个子带的底部具有几乎相同的能量,而第三子带的底部具有更高的能量(E_1≈E_2 << E_3)。在零平面磁场下,观察到第i个和第j个子带之间的磁间子带振荡(MISO),并遵循关系Δ_(ij)= E_j-E_i =khω_c,其中ω_c是回旋加速器频率,k是整数。平面磁场的应用会在MISO和相应的电子光谱中产生巨大变化。确定了三种制度。当hω_c<<Δ_(12)时,面内磁场会大大增加间隙Δ_(12),这与电子传播的半经典状态是一致的。相反,在强磁场hω_c>>Δ_(12)处,观察到电子谱随面内磁场的相对较弱的振荡变化。在hω_c≈Δ_(12)时,电子光谱通过磁击穿在这两种状态之间转变。在此过渡态中,具有奇数量子数k的MISO终止,而对应于偶数k的MISO连续演化为对应于hω_c>>Δ_(12)的高场态。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2016年第11期|115309.1-115309.12|共12页
  • 作者单位

    Physics Department, City College of the City University of New York, New York 10031, USA;

    Physics Department, City College of the City University of New York, New York 10031, USA;

    Physics Department, City College of the City University of New York, New York 10031, USA;

    Physics Department, City College of the City University of New York, New York 10031, USA;

    A. V. Rzhanov Institute of Semiconductor Physics, Novosibirsk 630090, Russia;

    A. V. Rzhanov Institute of Semiconductor Physics, Novosibirsk 630090, Russia and Novosibirsk State University, Novosibirsk 630090, Russia;

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