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首页> 外文期刊>Physical review, B >Magnetointersubband resistance oscillations in GaAs quantum wells placed in a tilted magnetic field
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Magnetointersubband resistance oscillations in GaAs quantum wells placed in a tilted magnetic field

机译:倾斜磁场中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 approximate to E-2 E-3). At zero in-plane magnetic fields, magnetointersubband oscillations (MISO) between the ith and j th subbands are observed and obey the relation Delta(ij) = E-j - E-i = k (h) over bar omega(c), where omega(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 (h) over bar omega(c) Delta(12), the in-plane magnetic field increases considerably the gap Delta(12), which is consistent with the semiclassical regime of electron propagation. In contrast, at strong magnetic fields (h) over bar omega(c) Delta(12) relatively weak oscillating variations of the electron spectrum with the in-plane magnetic field are observed. At (h) over bar omega(c) approximate to Delta(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 (h) over bar omega(c) Delta(12).
机译:研究了在倾斜磁场中具有三个人口子带的宽砷化镓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近似于E-2 E-3)。在平面内磁场为零时,观察到第i个和第j个子带之间的磁子带间振荡(MISO),并且在omega(c)上服从关系Delta(ij)= Ej-Ei = k(h),其中omega(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。在(h)超过barΩ(c) Delta(12)时,面内磁场会显着增大间隙Delta(12),这与电子传播的半经典机制是一致的。相比之下,在bar(Ω) Delta(12)上的强磁场(h)处,观察到电子光谱随面内磁场的相对较弱的振荡变化。在接近Delta(12)的bar(Ω)上方的(h)处,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不断演变成对应于在bar omega(c) Delta(12)上的(h)的高场态。

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