Conductor-Insulator Quantum Phase Transitions 2012
DOI: 10.1093/acprof:oso/9780199592593.003.0006
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Dynamical Mean-field Theories of Correlation and Disorder

Abstract: Dynamical mean-field theories of correlation and disorder 1.1 Mott transitions in clean and disordered systems 1.2 Mott-Anderson transitions: Typical Medium Theory 1.3 Mott-Anderson transitions: Statistical DMFT 1.4 Glassy behavior of correlated electrons 1.5 Beyond DMFT: loop expansion and diffusion modes 1.6 Acknowledgments References 1 Dynamical mean-field theories of correlation and disorder 1.1 Mott transitions in clean and disordered systems It is this fascination with the local and with the failures, no… Show more

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Cited by 5 publications
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“…Such a model is closely related to electronic models investigated in solid state physics [33], in particular correlated lattice electrons in random potentials; see, for example, refs. [34,35,36,37,38]. However, in solid state systems it is not possible (or, at least, not yet possible) to tune and manipulate spin-dependent potentials experimentally.…”
Section: Introductionmentioning
confidence: 99%
“…Such a model is closely related to electronic models investigated in solid state physics [33], in particular correlated lattice electrons in random potentials; see, for example, refs. [34,35,36,37,38]. However, in solid state systems it is not possible (or, at least, not yet possible) to tune and manipulate spin-dependent potentials experimentally.…”
Section: Introductionmentioning
confidence: 99%
“…(ii) After the phonon is replaced by the stochastic variable X j , the local electronic Green's function G j becomes a stochastic quantity itself, and one must solve the electron dynamics in the presence of a time-dependent disorder. This is achieved using a non-equilibrium generalization of statistical DMFT [39][40][41]. In the simulations, we explicitly treat 128 representative sites on the A and B sublattices, which give access on the full distribution of local properties.…”
mentioning
confidence: 99%
“…We solve Eq. ( 1) on a lattice of N s sites, using realspace DMFT [18][19][20], an extension of DMFT [8] introduced to treat inhomogeneous system. The key approximation is to assume a local, albeit site-dependent, self-energy matrix Σij = δ ij Σi .…”
mentioning
confidence: 99%