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Many-body delocalization transition and relaxation in a quantum dot  [PDF]
I. V. Gornyi,A. D. Mirlin,D. G. Polyakov
Physics , 2015,
Abstract: We revisit the problem of quantum localization of many-body states in a quantum dot and the associated problem of relaxation of an excited state in a finite correlated electron system. We determine the localization threshold for the eigenstates in Fock space. We argue that the localization-delocalization transition (which manifests itself, e.g., in the statistics of many-body energy levels) becomes sharp in the limit of a large dimensionless conductance (or, equivalently, in the limit of weak interaction). We also analyze the temporal relaxation of quantum states of various types (a "hot-electron state", a "typical" many-body state, and a single-electron excitation added to a "thermal state") with energies below, at, and above the transition.
Nonuniversal transmission phase lapses through a quantum dot: An exact-diagonalization of the many-body transport problem  [PDF]
Leslie O. Baksmaty,Constantine Yannouleas,Uzi Landman
Physics , 2008, DOI: 10.1103/PhysRevLett.101.136803
Abstract: Systematic trends of nonuniversal behavior of electron transmission phases through a quantum dot, with no phase lapse for the transition N=1 -> N=2 and a lapse of pi for the N=2 -> N=3 transition, are predicted, in agreement with experiments, from many-body transport calculations involving exact diagonalization of the dot Hamiltonian. The results favor shape anisotropy of the dot and strong e-e repulsion with consequent electron localization, showing dependence on spin configurations and the participation of excited doorway transmission channels.
Spectroscopic signatures of many-body interactions and delocalized states in self-assembled lateral quantum dot molecules  [PDF]
X. Zhou,S. Sanwlani,W. Liu,J. H. Lee,Zh. M. Wang,G. Salamo,M. F. Doty
Physics , 2011, DOI: 10.1103/PhysRevB.84.205411
Abstract: Lateral quantum dot molecules consist of at least two closely-spaced InGaAs quantum dots arranged such that the axis connecting the quantum dots is perpendicular to the growth direction. These quantum dot complexes are called molecules because the small spacing between the quantum dots is expected to lead to the formation of molecular-like delocalized states. We present optical spectroscopy of ensembles and individual lateral quantum dot molecules as a function of electric fields applied along the growth direction. The results allow us to characterize the energy level structure of lateral quantum dot molecules and the spectral signatures of both charging and many-body interactions. We present experimental evidence for the existence of molecular-like delocalized states for electrons in the first excited energy shell.
Exact scattering eigenstates, many-body bound states, and nonequilibrium current of an open quantum dot system  [PDF]
Akinori Nishino,Takashi Imamura,Naomichi Hatano
Physics , 2009, DOI: 10.1103/PhysRevLett.102.146803
Abstract: We obtain an exact many-body scattering eigenstate in an open quantum dot system. The scattering state is not in the form of the Bethe eigenstate in the sense that the wave-number set of the incoming plane wave is not conserved during the scattering and many-body bound states appear. By using the scattering state, we study the average nonequilibrium current through the quantum dot under a finite bias voltage. The current-voltage characteristics that we obtained by taking the two-body bound state into account is qualitatively similar to several known results.
Nonequilibrium dynamics in an optical transition from a neutral quantum dot to a correlated many-body state  [PDF]
F. Haupt,S. Smolka,M. Hanl,W. Wüster,J. Miguel-Sanchez,A. Weichselbaum,J. von Delft,A. Imamoglu
Physics , 2013, DOI: 10.1103/PhysRevB.88.161304
Abstract: We investigate the effect of many-body interactions on the optical absorption spectrum of a charge-tunable quantum dot coupled to a degenerate electron gas. A constructive Fano interference between an indirect path, associated with an intra dot exciton generation followed by tunneling, and a direct path, associated with the ionization of a valence-band quantum dot electron, ensures the visibility of the ensuing Fermi-edge singularity despite weak absorption strength. We find good agreement between experiment and renormalization group theory, but only when we generalize the Anderson impurity model to include a static hole and a dynamic dot-electron scattering potential. The latter highlights the fact that an optically active dot acts as a tunable quantum impurity, enabling the investigation of a new dynamic regime of Fermi-edge physics.
Comparison of EIT schemes in semiconductor quantum dot structures: Impact of many-body interactions  [PDF]
J. Houmark,T. R. Nielsen,J. Mork,A. -P. Jauho
Physics , 2009, DOI: 10.1103/PhysRevB.79.115420
Abstract: We investigate the impact of many-body interactions on group-velocity slowdown achieved via electromagnetically induced transparency in quantum dots using three different coupling-probe schemes (ladder, V, and Lambda, respectively). We find that for all schemes many-body interactions have an important impact on the slow light properties. In the case of the Lambda and V schemes, the minimum required coupling power to achieve slow light is significantly reduced by many-body interactions. V type schemes are found to be generally preferable due to a favorable redistribution of carriers in energy space.
Many-body excitations in tunneling current spectra of a few-electron quantum dot  [PDF]
D. V. Melnikov,T. Fujisawa,D. G. Austing,S. Tarucha,J. -P. Leburton
Physics , 2007, DOI: 10.1103/PhysRevB.77.165340
Abstract: Inherent asymmetry in the tunneling barriers of few-electron quantum dots induces intrinsically different tunneling currents for forward and reverse source-drain biases in the non-linear transport regime. Here we show that in addition to spin selection rules, overlap matrix elements between many-body states are crucial for the correct description of tunneling transmission through quantum dots at large magnetic fields. Signatures of excited (N-1)-electron states in the transport process through the N-electron system are clearly identified in the measured transconductances. Our analysis clearly confirms the validity of single-electron quantum transport theory in quantum dots.
Anisotropic magnetic field dependence of many-body enhanced electron tunnelling through a quantum dot  [PDF]
E. E. Vdovin,Yu. N. Khanin,O. Makarovsky,A. Patane,L. Eaves,M. Henini,C. J. Mellor,K. A. Benedict,R. Airey
Physics , 2007,
Abstract: We investigate the effect of an applied magnetic field on resonant tunneling of electrons through the bound states of self-assembled InAs quantum dots (QDs) embedded within an (AlGa)As tunnel barrier. At low temperatures (no more than 2 K), a magnetic field B applied either parallel or perpendicular to the direction of current flow causes a significant enhancement of the tunnel current. For the latter field configuration, we observe a strong angular anisotropy of the enhanced current when B is rotated in the plane of the quantum dot layer. We attribute this behavior to the effect of the lowered symmetry of the QD eigenfunctions on the electron-electron interaction.
Quantum phases in artificial molecules  [PDF]
Massimo Rontani,Filippo Troiani,Ulrich Hohenester,Elisa Molinari
Physics , 2001, DOI: 10.1016/S0038-1098(01)00226-5
Abstract: The many-body state of carriers confined in a quantum dot is controlled by the balance between their kinetic energy and their Coulomb correlation. In coupled quantum dots, both can be tuned by varying the inter-dot tunneling and interactions. Using a theoretical approach based on the diagonalization of the exact Hamiltonian, we show that transitions between different quantum phases can be induced through inter-dot coupling both for a system of few electrons (or holes) and for aggregates of electrons and holes. We discuss their manifestations in addition energy spectra (accessible through capacitance or transport experiments) and optical spectra.
Many-Body Approch to Spin-Dependent Transport in Quantum Dot Systems  [PDF]
J. Fransson,O. Eriksson,I. Sandalov
Physics , 2002, DOI: 10.1103/PhysRevLett.88.226601
Abstract: By means of a diagram technique for Hubbard operators we show the existence of a spin-dependent renormalization of the localized levels in an interacting region, e.g. quantum dot, modeled by the Anderson Hamiltonian with two conduction bands. It is shown that the renormalization of the levels with a given spin direction is due to kinematic interactions with the conduction sub-bands of the opposite spin. The consequence of this dressing of the localized levels is a drastically decreased tunneling current for ferromagnetically ordered leads compared to that of paramagnetically ordered leads. Furthermore, the studied system shows a spin-dependent resonant tunneling behaviour for ferromagnetically ordered leads.
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