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The distribution function P(j) of the microscopic energy flux, j, inequilibrium state is studied. It is observed that P(j) has a broad peak insmall j regime and a stretched-exponential decay for large j. The peakstructure originates in a potential advection term and energy transfer termbetween the particles. The stretched exponential tail comes from the momentumenergy advection term.Comment: 5 pages, 2 figure

Distribution of Microscopic Energy Flux in Equilibrium State