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首页> 外文期刊>Physical Review, B. Condensed Matter >Electron-hole separation studies near the nu=1 quantum Hall state in modulation-doped GaAs/(Al,Ga)As single heterojunctions in high magnetic fields - art. no. 195302
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Electron-hole separation studies near the nu=1 quantum Hall state in modulation-doped GaAs/(Al,Ga)As single heterojunctions in high magnetic fields - art. no. 195302

机译:高磁场中掺有调制的GaAs /(Al,Ga)As单异质结中nu = 1量子霍尔态附近的电子-空穴分离研究-艺术。没有。 195302

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摘要

Magnetophotoluminescence (MPL) studies as a function of carrier concentration are reported for a series of very high mobility n-type modulation-doped GaAs/(Al,Ga)As single heterojunctions. The measurements were made in high magnetic fields to similar to 60 T and at temperatures in the 0.4-2.1 K range. At low fields (nu >2), the MPL recombination is dominated a free carrierlike excitonic transition as an energy close to the free exciton in bulk GaAs. The energy and intensity of this excitation undergoes Shubnikov-de Haas-type oscillations at even integer filling factors (nu> 2) with increasing field. At nu= 2(-), an second strong exciton transition appears at a lower energy primarily in sigma (-) polarization due to a spin up arrow electron recombining with a valence-band hole. It rapidly gains intensity between 2> nu> 1, but disappears at nu= 1(+). At nu= 1(-) another redshifted transition emerges that has been described as a recombination of an electron in an initial "free hole state." Its intensity in sigma (-) polarization increases and reaches a maximum between 1> nu >1/3. Such behavior becomes more pronounced as the carrier density increases. The redshift at nu= 1 has been correlated with recent theoretical models describing the theory of photoluminescence of two-dimensional electron systems. It has been used to determine the electron-hole separation as a function of carrier concentration. [References: 31]
机译:磁光致发光(MPL)研究作为载流子浓度的函数,报告了一系列非常高迁移率的n型调制掺杂GaAs /(Al,Ga)As单异质结。在类似于60 T的强磁场中以及在0.4-2.1 K范围内的温度下进行测量。在低场(nu> 2)下,MPL重组以自由载流子样激子跃迁为主,其能量接近块状GaAs中的自由激子。随着场的增加,这种激发的能量和强度在偶数整数填充因子(nu> 2)处经历Shubnikov-de Haas型振荡。在nu = 2(-)处,由于自旋向上的箭头电子与价带空穴重组,第二个强激子跃迁以较低的能量出现在sigma(-)极化中。它迅速获得2> nu> 1之间的强度,但在nu = 1(+)时消失。在nu = 1(-)处,出现了另一个红移跃迁,该跃迁已描述为初始“自由空穴态”下电子的复合。它的σ(-)极化强度增加,并在1> nu> 1/3之间达到最大值。随着载流子密度的增加,这种行为变得更加明显。 nu = 1处的红移已与描述二维电子系统光致发光理论的最新理论模型相关。它已被用来确定作为载流子浓度的函数的电子-空穴分离。 [参考:31]

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