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首页> 外文期刊>The Journal of Chemical Physics >Single-particle and collective excitations in quantum wires made up of vertically stacked quantum dots: Zero magnetic field
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Single-particle and collective excitations in quantum wires made up of vertically stacked quantum dots: Zero magnetic field

机译:由垂直堆叠的量子点组成的量子线中的单粒子和集体激发:零磁场

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We report on the theoretical investigation of the elementary electronic excitations in a quantum wire made up of vertically stacked self-assembled InAs/GaAs quantum dots. The length scales (of a few nanometers) involved in the experimental setups prompt us to consider an infinitely periodic system of two-dimensionally confined (InAs) quantum dot layers separated by GaAs spacers. The resultant quantum wire is characterized by a two-dimensional harmonic confining potential in the x-y plane and a periodic (Kronig-Penney) potential along the z (or the growth) direction within the tight-binding approximation. Since the wells and barriers are formed from two different materials, we employ the Bastards boundary conditions in order to determine the eigenfunctions along the z direction. These wave functions are then used to generate the Wannier functions, which, in turn, constitute the legitimate Bloch functions that govern the electron dynamics along the direction of periodicity. Thus, the Bloch functions and the Hermite functions together characterize the whole system. We then make use of the Bohm-Pines' (full) random-phase approximation in order to derive a general nonlocal, dynamic dielectric function. Thus, developed theoretical framework is then specified to work within a (lowest miniband and) two-subband model that enables us to scrutinize the single-particle as well as collective responses of the system. We compute and discuss the behavior of the eigenfunctions, band-widths, density of states, Fermi energy, single-particle and collective excitations, and finally size up the importance of studying the inverse dielectric function in relation with the quantum transport phenomena. It is remarkable to notice how the variation in the barrier- and well-widths can allow us to tailor the excitation spectrum in the desired energy range. Given the advantage of the vertically stacked quantum dots over the planar ones and the foreseen applications in the single-electron devices and in the quantum computation, it is quite interesting and important to explore the electronic, optical, and transport phenomena in such systems.
机译:我们报告了由垂直堆叠的自组装InAs / GaAs量子点组成的量子线中基本电子激发的理论研究。实验装置中涉及的长度尺度(几纳米)促使我们考虑一个无限周期的系统,该系统由GaAs间隔物分隔开的二维约束(InAs)量子点层。最终的量子线的特征是在x-y平面中具有二维谐波约束电势,并且在紧密束缚近似中沿z(或生长)方向具有周期性(Kronig-Penney)电势。由于阱和势垒是由两种不同的材料形成的,因此我们采用Bastards边界条件来确定沿z方向的本征函数。然后,这些波函数用于生成Wannier函数,后者又构成合法的Bloch函数,该函数控制沿周期性方向的电子动力学。因此,Bloch函数和Hermite函数共同构成整个系统的特征。然后,我们利用Bohm-Pines(完全)随机相位逼近来得出一般的非局部动态介电函数。因此,然后指定了发达的理论框架,以在(最低的最小频带和)两个子频带模型中工作,这使我们能够检查系统的单粒子以及集体响应。我们计算并讨论了本征函数的行为,带宽,状态密度,费米能量,单粒子和集体激发,最后确定了研究与量子传输现象有关的逆介电函数的重要性。值得注意的是,势垒宽度和阱宽度的变化如何使我们能够在所需的能量范围内调整激发光谱。鉴于垂直堆积的量子点相对于平面量子点的优势以及可预见的在单电子器件和量子计算中的应用,探索此类系统中的电子,光学和传输现象非常有趣且重要。

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