Mesoscopic Effects in Metal Grains and Quantum Dots

金属晶粒和量子点的介观效应

• 批准号: 0334499
• 负责人: Piet Brouwer
• 金额: $ 27.6万
• 依托单位: Cornell University
• 依托单位国家: 美国
• 项目类别: Continuing Grant
• 财政年份: 2003
• 资助国家: 美国
• 起止时间: 2003-12-01 至 2007-11-30
• 项目状态: 已结题
• 来源: https://www.nsf.gov/awardsearch/showAward?AWD_ID=0334499&HistoricalAwards=false
• 关键词: Mesoscopic; Effects; Metal; Grains; Quantum

Single-particle properties of a small metal grain or semiconductor quantum dot can be described by random-matrix theory: energy levels and wavefunctions have the same statistics as eigenvalues and eigenvectors of a large hermitian matrix with real, complex or quaternion numbers, depending on the presence or absence of time-reversal symmetry and spin-rotation symmetry. Kurland, Aleiner and Altshuler proposed that electron-electron interaction effects in this "random matrix limit" are described by a "universal interaction Hamiltonian," which has only interaction terms that are invariant under the symmetry transformations of the random matrix ensemble. These interactions are self-averaging and non-random, hence the label "universal." The first part of this research addresses the role of interactions when symmetries are "partially" broken, e.g., in the presence of spin-orbit scattering that is too weak to fully randomize the electron spin within the time to ergodically explore the grain or dot. For such "partially broken symmetries," the interaction Hamiltonian is a random quantity, since interaction matrix elements are no longer self-averaging. Such fluctuations of the interaction Hamiltonian may effect g factors of individual electronic levels in metal grains, or the suppression of superconducting fluctuations in a superconducting metal grain near the critical temperature. This research also addresses the Stoner instability in metal grains and the ferromagnetic state formed beyond the instability. Both the approach of the instability and the ferromagnetic state itself display interesting mesoscopic phenomena if spin-orbit scattering is present. With strong spin-orbit coupling, exchange interaction matrix elements are small and violate the symplectic symmetry of random matrix theory, yet, they are many, and trigger the formation of a ferromagnetic state irrespective of the spin-orbit scattering strength. Hence, this instability provides the context for a controlled calculation how interactions may drive systems away from the random matrix. For a ferromagnet, randomness in the spatial part of the wavefunction couples to the magnetization through spin-orbit coupling, giving rise to a "mesoscopic" component of the anisotropy energy.The second part of the research deals with time-dependent transport in quantum dots. Time-dependent transport has both practical and fundamental interest. Practical interest arises because speed is a concern in most electronic devices. Time-dependent transport (as well as nonlinear response) is of fundamental interest because electron-electron interactions play a much more important role for time-dependent transport than for time-independent transport. A detailed calculation will be done that should give insight how the capacitive charging energy affects phase-coherent time-dependent transport in quantum dots connected to electrodes via point contacts. Although charge quantization is lifted in those systems, Coulomb blockade continues to be important for transport properties.Besides advancing the fundamental scientific understanding of metals and semiconductors on the nanometer scale, the research will provide training material to help theory graduate students develop into well-rounded condensed matter physicists. Undergraduates will also participate in the research. Graduate students will also participate in the outreach activities of the Cornell MRSEC.%%%This theoretical research will address a number of issues relating to the properties of nanoscale metals and semiconductors. The research has very fundamental ramifications and, as is typical of this field, practical applications are near.Besides advancing the fundamental scientific understanding of metals and semiconductors on the nanometer scale, the research will provide training material to help theory graduate students develop into well-rounded condensed matter physicists. Undergraduates will also participate in the research. Graduate students will also participate in the outreach activities of the Cornell MRSEC.***

小金属颗粒或半导体量子点的单粒子性质可以用随机矩阵理论来描述：能级和波函数与具有真实的、复数或四元数的大厄米矩阵的本征值和本征向量具有相同的统计特性，这取决于时间反演对称性和自旋旋转对称性的存在或不存在。 Kurland、Aleiner和Altshirt提出，在这个“随机矩阵极限”中的电子-电子相互作用效应可以用一个“通用相互作用哈密顿量”来描述，它只有在随机矩阵系综的对称变换下不变的相互作用项。 这些相互作用是自平均和非随机的，因此被称为“普适的”。“这项研究的第一部分讨论了当对称性“部分”被打破时相互作用的作用，例如，在自旋-轨道散射的存在下，该散射太弱而不能在遍历地探索颗粒或点的时间内完全随机化电子自旋。 对于这种“部分破缺的对称性”，相互作用哈密顿量是一个随机量，因为相互作用矩阵元素不再是自平均的。 这种相互作用哈密顿量的涨落可能影响金属颗粒中单个电子能级的g因子，或在临界温度附近抑制超导金属颗粒中的超导涨落。本研究还讨论了金属晶粒中的Stoner不稳定性以及在不稳定性之外形成的铁磁态。 如果存在自旋轨道散射，则不稳定性和铁磁态本身的方法都显示出有趣的介观现象。 在强自旋-轨道耦合的情况下，交换相互作用矩阵元很小并且违反随机矩阵理论的辛对称性，然而，它们很多，并且触发铁磁状态的形成，而不管自旋-轨道散射强度如何。 因此，这种不稳定性为受控计算提供了背景，相互作用如何使系统远离随机矩阵。 对于铁磁体，波函数空间部分的随机性通过自旋-轨道耦合耦合到磁化强度，产生各向异性能量的“介观”分量。研究的第二部分涉及量子点中的时间相关输运。 含时输运具有实际意义和根本意义。 由于速度是大多数电子设备的关注点，因此引起了实际兴趣。 时间依赖性输运（以及非线性响应）是基本的兴趣，因为电子-电子相互作用的时间依赖性输运比时间无关的输运发挥更重要的作用。 将进行详细的计算，应该可以洞察电容充电能量如何影响通过点接触连接到电极的量子点中的相位相干时变输运。 虽然这些系统中的电荷量子化被解除，但库仑阻塞对输运性质仍然很重要。除了在纳米尺度上推进对金属和半导体的基础科学理解外，这项研究还将提供培训材料，帮助理论研究生发展成为全面的凝聚态物理学家。 本科生也将参与研究。 研究生还将参加康奈尔大学MRSEC的外展活动。%这项理论研究将解决一些与纳米金属和半导体性质有关的问题。 该研究具有非常基础的分支，并且作为该领域的典型，实际应用是接近的。除了推进纳米尺度上的金属和半导体的基础科学理解之外，该研究还将提供培训材料，帮助理论研究生发展成为全面的凝聚态物理学家。 本科生也将参与研究。 研究生还将参加康奈尔大学MRSEC的外联活动。