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A. Wobst

Publications and source records attributed to A. Wobst.

5 recordsLinked to original sources
arXiv2006

Scrambling of Hartree-Fock Levels as a universal Brownian-Motion Process

We study scrambling of the Hartree-Fock single-particle levels and wave functions as electrons are added to an almost isolated diffusive or chaotic quantum dot with electron-electron interactions. We use the generic framework of the induced two-body ensembles where the randomness of the two-body interaction matrix elements is induced by the randomness of the eigenfunctions of the chaotic or diffusive single-particle Hamiltonian. After an appropriate scaling of the number of added electrons, the scrambling of both the HF levels and wave functions is described by a universal function each. These functions can be derived from a parametric random matrix process of the Brownian-motion type. An exception to this universality occurs when an empty level just gets filled, in which case scrambling is delayed by one electron. An explanation of these results is given in terms of a generalized Koopmans' approach.

cond-mat.mes-hall↗
arXiv2004

Disordered mesoscopic systems with interactions: induced two-body ensembles and the Hartree-Fock approach

We introduce a generic approach to study interaction effects in diffusive or chaotic quantum dots in the Coulomb blockade regime. The randomness of the single-particle wave functions induces randomness in the two-body interaction matrix elements. We classify the possible induced two-body ensembles, both in the presence and absence of spin degrees of freedom. The ensembles depend on the underlying space-time symmetries as well as on features of the two-body interaction. Confining ourselves to spinless electrons, we then use the Hartree-Fock (HF) approximation to calculate HF single-particle energies and HF wave functions for many realizations of the ensemble. We study the statistical properties of the resulting one-body HF ensemble for a fixed number of electrons. In particular, we determine the statistics of the interaction matrix elements in the HF basis, of the HF single-particle energies (including the HF gap between the last occupied and the first empty HF level), and of the HF single-particle wave functions. We also study the addition of electrons, and in particular the distribution of the distance between successive conductance peaks and of the conductance peak heights.

cond-mat.mes-hall↗
arXiv2000

Random matrix model for quantum dots with interactions and the conductance peak spacing distribution

We introduce a random interaction matrix model (RIMM) for finite-size strongly interacting fermionic systems whose single-particle dynamics is chaotic. The model is applied to Coulomb blockade quantum dots with irregular shape to describe the crossover of the peak spacing distribution from a Wigner-Dyson to a Gaussian-like distribution. The crossover is universal within the random matrix model and is shown to depend on a single parameter: a scaled fluctuation width of the interaction matrix elements. The crossover observed in the RIMM is compared with the results of an Anderson model with Coulomb interactions.

cond-mat.mes-hall↗
arXiv2000

Interaction effects on the conductance peak height statistics in quantum dots

A random interaction matrix model is used to study the statistics of conductance peak heights in Coulomb blockade quantum dots. When the single-particle dynamics conserves time-reversal symmetry, the peak height statistics is insensitive to the interaction strength. But when the single-particle dynamics breaks time-reversal symmetry, the peak height statistics exhibits a crossover from unitary to orthogonal symmetry as the interaction strength increases. This crossover is driven by the time-reversal symmetry of the interaction. Our random interaction matrix model describes features of both the measured peak height and peak spacing statistics.

cond-mat.mes-hall↗