000019666 001__ 19666 000019666 005__ 20230426083032.0 000019666 0247_ $$2DOI$$a10.1103/PhysRevB.85.024204 000019666 0247_ $$2WOS$$aWOS:000299116400006 000019666 0247_ $$2Handle$$a2128/10883 000019666 037__ $$aPreJuSER-19666 000019666 041__ $$aeng 000019666 082__ $$a530 000019666 084__ $$2WoS$$aPhysics, Condensed Matter 000019666 1001_ $$0P:(DE-Juel1)130955$$aSchober, H.R.$$b0$$uFZJ 000019666 245__ $$aModeling aging rates in a simple glass and its melt 000019666 260__ $$aCollege Park, Md.$$bAPS$$c2012 000019666 300__ $$a024204 000019666 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000019666 3367_ $$2DataCite$$aOutput Types/Journal article 000019666 3367_ $$00$$2EndNote$$aJournal Article 000019666 3367_ $$2BibTeX$$aARTICLE 000019666 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000019666 3367_ $$2DRIVER$$aarticle 000019666 440_0 $$04919$$aPhysical Review B$$v85$$x1098-0121$$y2 000019666 500__ $$3POF3_Assignment on 2016-02-29 000019666 500__ $$aRecord converted from VDB: 12.11.2012 000019666 520__ $$aWe calculated with a molecular dynamics simulation the aging rates in a binary Lennard-Jones glass and its undercooled melt. At temperatures above the mode coupling theory (MCT) critical temperature T-c, pressure or volume, internal energy, and diffusivity age with the same rate. Below T-c we see a split of the aging rates into a fast one for the diffusivity and a much slower one for pressure or volume and internal energy. The latter aging rate is roughly proportional to the diffusivity. The observed stretched exponential behavior is shown to stem from the faster aging of the diffusivity. Aging of of internal energy and pressure proceeds exponentially with the mean-square displacement. 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