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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

David Logan

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  • Rudolf Peierls Centre for Theoretical Physics
david.logan@chem.ox.ac.uk
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General discussion

Faraday Discussions of the Chemical Society 85 (1988) 391-396

Authors:

MCR Symons, S Tomoda, T Clark, ML Klein, BM Odintsov, PG Wolynes, M Sprik, JP Devlin, DE Logan, M Marchi
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THE DENSITY OF STATES OF A SPATIALLY DISORDERED TIGHT-BINDING MODEL

JOURNAL OF PHYSICS C-SOLID STATE PHYSICS 21:34 (1988) 5773-5795

Authors:

DE LOGAN, MD WINN
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M//xTi//2// minus //x.

Disord Semicond (1987)

Authors:

PM Lambert, MR Harrison, DE Logan, PP Edwards

Abstract:

The possible nature of the composition induced transition from superconductor to semiconductor in a system with obvious crystalline order - in association with equally obvious electronic disorder - is considered. Topics discussed include: structural parameters, superconductivity, IR spectra, the nature of superconductor-semiconductor transition, as well as percolation and disproportionation.

The microstructure of colloidal silver: Evidence for a polytetrahedral growth sequence

Journal of the Chemical Society, Chemical Communications (1987) 1264-1266

Authors:

DG Duff, AC Curtis, PP Edwards, DA Jefferson, BFG Johnson, DE Logan

Abstract:

High resolution electron microscopy of very small (ca. 40 Å diameter) colloidal silver particles established their decahedral morphology.
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Dephasing and Anderson localization in topologically disordered systems

Physical Review B 36:8 (1987) 4135-4147

Authors:

DE Logan, PG Wolynes

Abstract:

A simple theory is developed to describe the interplay between Anderson localization and dephasing mechanisms (such as inelastic electron- or exciton-phonon coupling), within the framework of a tight-binding model of spatially disordered systems. Self-consistency is enforced by demanding that only the most probable value of the imaginary part of the site self-energy be self-consistently determined. Dephasing interactions are characterized simply by an energy-independent dephasing rate. When the dephasing rate vanishes the pure localization problem may be examined as the transition is approached from either the localized or the extended regimes; mobility-edge trajectories may thereby be located. In the limit of rapid dephasing the theory correlates with the usual master-equation treatments of incoherent transport. For sufficiently large disorder a nonmonotonic but continuous crossover from coherent to incoherent transport is in general predicted. The problem of Mooij correlation, viewed as a weak-delocalization phenomenon, is also examined: it is suggested that the correlation is not universal as has frequently been supposed. © 1987 The American Physical Society.
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