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  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
411

Polycrystalline silicon thin-film transistors for large-scale microelectronics

Coxon, Penelope Anne January 1990 (has links)
No description available.
412

Electron tunnelling in metal-oxide-silicon structures

Owen, Michael Paul January 1991 (has links)
No description available.
413

Superconducting magnetic bearings

Coombs, Timothy A. January 1995 (has links)
No description available.
414

Local field effects and plasmon excitations in covalent semiconductors

Oliveira, L. E. M. C. de January 1981 (has links)
No description available.
415

Electrical properties of small molecules

Williams, J. H. January 1980 (has links)
No description available.
416

The physical processes in organic semiconducting polymer devices

Burroughes, Jeremy Henley January 1989 (has links)
No description available.
417

Electronic states of epitaxial magnetic layers : metastable FCC iron and cobalt on copper (001)

Almeida, Fabio J. D. January 1990 (has links)
No description available.
418

Electronic properties of some low dimensional systems

Read, A. J. January 1991 (has links)
No description available.
419

A study of 3He films using SQUID NMR

Dyball, Helen Catherine Jane January 2001 (has links)
No description available.
420

Molecular dynamics simulations of calamitic and discotic liquid crystals

De Luca, Marc Dominic January 1997 (has links)
Significant progress has been made in recent years in modelling liquid crystal phases using the Monte Carlo and molecular dynamics simulation techniques. We describe the technique of molecular dynamics in the microcanonical ensemble that we have used in simulations of liquid crystal systems. A review and discussion of some of the important simulations that have been performed to date on non-spherical hard particle models, soft anisotropic single site models, and realistic atom-atom based models is presented. We report the results of molecular dynamics simulation studies of a system of particles interacting via an anisotropic potential proposed by Luckhurst and Romano, scaled by part of the well depth formulation employed by Gay and Berne. The resultant hybrid Gay-Berne Luckhurst-Romano (HGBLR) potential has an approximately spherical hard core with anisotropic long range attractive interactions with a dependency on the intermolecular vector joining a pair of sites. The spherical hard core nature of individual HGBLR centres notwithstanding we have parameterised single-site HGBLR centres to represent both calarnitic and discotic mesogens. Both systems are shown to exhibit a range of mesophases on cooling from the isotropic liquid to form a crystal, including uniaxial-nematic and columnar-like phases. Unlike previous hard particle studies these ordered phases obtain because of the presence of the long range attractive interactions. A comparison between the different structures formed with the two different parameterisations is presented including graphical representations of the simulation cell . In order to more closely represent the short range anisotropic interactions of real mesogens, a 3-HGBLR-site model has been parameterised to represent the mesogen para-terphenyl. Details of the parameterisation are discussed. Two versions of this model, a twisted central site 3-HGBLR-site site model obtained from a molecular mechanics minimum energy conformation of para-terphenyl, and an all coplanar 3-HGBLR-site site model have been studied using the molecular dynamics technique. The resultant models are found to be biaxial unlike previous anisotropic single site studies utilising soft potentials. Both models appear to exhibit a variety of uniaxial and biaxial mesophases but inclusion of the twisted site appears to promote the formation of biaxial phases. A comparison of the two models is made.

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