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Geometric Thermodynamics
[stub]
2019
Figshare
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Here we introduce a non-commutative extension to statistical physics granting it the ability to associate an entropy to arbitrary space-times. Generally speaking, statistical physics connects a set Q of 'microstates' (a.k.a the microscopic description) to a set of functions on Q (a.k.a. the bulk state) by the use of Lagrange multipliers, and under the principle of maximum entropy. In the present case, the 'microscopic' object of study is the space-time event, the bulk state is the space-time
doi:10.6084/m9.figshare.8079665.v4
fatcat:owdzkblpnzac5lrt57fra4dxji