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For a hard-sphere fluid this is always negative. Inset: Difference between the corresponding vibrational part of the entropy of the amorphous state and the crystal entropy. Dependence of the configurational entropy on amorphous structures of a hard-sphere fluid Arijit Mondal, Leishangthem Premkumar, and Shankar P.

Das Phys.

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INHOMOGENEOUS RANDOM SYSTEMS

E 96 , — Published 12 July Abstract The free energy of a hard-sphere fluid for which the average energy is trivial signifies how its entropy changes with packing. Research Areas. Classical statistical mechanics Entropy Jamming Thermodynamics Transition temperature. Issue Vol. Authorization Required.

Statistical Mechanics Lecture 4

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DETERMINISTIC SPONTANEOUS APPEARANCE OF TRAFFIC JAMS IN SLIGHTLY INHOMOGENEOUS TRAFFIC FLOW

X Rev. A Phys. Bacterial growth: a statistical physicist's guide DOI. Reduced adhesion between cells and substrate confers selective advantage in bacterial colonies DOI.

Nature Communications

Mechanical interactions in bacterial colonies and the surfing probability of beneficial mutations DOI. An exactly solvable, spatial model of mutation accumulation in cancer DOI.


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Localization and Glassy Dynamics Of Many-Body Quantum Systems

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An exclusion process on a tree with constant aggregate hopping rate DOI. Mechanically driven growth of quasi-two dimensional microbial colonies DOI. Quantum widening of a causal dynamical triangulations universe DOI.

Staff Publications

Spectrum of the product of independent random Gaussian matrices DOI. Mass condensation on networks DOI. Mass condensation in one dimension with pair-factorized steady states DOI. Pair-factorized steady states on arbitrary graphs DOI.