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J. M. Kosterlitz

Researcher at Brown University

Publications -  84
Citations -  12872

J. M. Kosterlitz is an academic researcher from Brown University. The author has contributed to research in topics: Classical XY model & Critical exponent. The author has an hindex of 32, co-authored 82 publications receiving 11699 citations. Previous affiliations of J. M. Kosterlitz include McGill University & University of Birmingham.

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Ordering, metastability and phase transitions in two-dimensional systems

TL;DR: In this article, a new definition of order called topological order is proposed for two-dimensional systems in which no long-range order of the conventional type exists, and the possibility of a phase transition characterized by a change in the response of the system to an external perturbation is discussed in the context of a mean field type of approximation.
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The critical properties of the two-dimensional xy model

TL;DR: In this paper, the critical properties of the xy model with nearest-neighbour interactions on a two-dimensional square lattice were studied by a renormalization group technique, and the correlation length is found to diverge faster than any power of the deviation from the critical temperature.
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Universal Jump in the Superfluid Density of Two-Dimensional Superfluids

TL;DR: In this article, it was shown that a universal jump in the superfluid density of two-dimensional planar magnets and liquid crystals occurs when the phase transition is approached from below.
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Long range order and metastability in two dimensional solids and superfluids. (Application of dislocation theory)

TL;DR: In this paper, it was shown that the rigidity modulus is nonzero at the transition temperature of a two-dimensional superfluid, and that the superfluid density is not zero at any temperature.
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Growth in a restricted solid-on-solid model.

TL;DR: In this article, extensive simulations of growth in a stochastic ballistic deposition model on a (d-1)-dimensional substrate with a constraint on neighboring interface heights are described, and the interface width obeys scaling even for small systems and grows as ${t}^{\ensuremath{\beta}}$ with \ensureMath{\beta}=1/(d+1).