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On the Local Equilibrium Condition
High Energy Physics - Theory · Submitted 14 Nov 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is shown that the principle of maximal entropy does not always lead to physical states if it is applied to relativistic quantum field theories.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
A physical system is in local equilibrium if it cannot be distinguished from a global equilibrium by ``infinitesimally localized measurements''. This should be a natural characterization of local equilibrium, but the problem is to give a precise meaning to the qualitative phrase ``infinitesimally localized measurements''. A solution is suggested in form of a Local Equilibrium Condition, which can be applied to linear relativistic quantum field theories but not directly to selfinteracting quantum fields. The concept of local temperature resulting from LEC is compared to an old approach to local temperature based on the principle of maximal entropy. It is shown that the principle of maximal entropy does not always lead to physical states if it is applied to relativistic quantum field theories.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A physical system is in local equilibrium if it cannot be distinguished from a global equilibrium by ``infinitesimally localized measurements''. | background 1.00 | 0.12 | 0.08 | asserted 1.00 |
| s1 | This should be a natural characterization of local equilibrium, but the problem is to give a precise meaning to the qualitative phrase ``infinitesimally localized measurements''. | gap 0.87 | 0.13 | 0.03 | asserted 0.67 |
| s2 | A solution is suggested in form of a Local Equilibrium Condition, which can be applied to linear relativistic quantum field theories but not directly to selfinteracting quantum fields. | contribution 0.90 | 0.75 | 0.37 | hedged possibility 0.77 |
| s3 | The concept of local temperature resulting from LEC is compared to an old approach to local temperature based on the principle of maximal entropy. | contribution 0.80 | 0.72 | 0.08 | asserted 0.96 |
| s4 | It is shown that the principle of maximal entropy does not always lead to physical states if it is applied to relativistic quantum field theories. | result 0.99 | 0.81 | 0.29 | asserted 1.00 |
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Original abstract
A physical system is in local equilibrium if it cannot be distinguished from a global equilibrium by ``infinitesimally localized measurements''. This should be a natural characterization of local equilibrium, but the problem is to give a precise meaning to the qualitative phrase ``infinitesimally localized measurements''. A solution is suggested in form of a Local Equilibrium Condition, which can be applied to linear relativistic quantum field theories but not directly to selfinteracting quantum fields. The concept of local temperature resulting from LEC is compared to an old approach to local temperature based on the principle of maximal entropy. It is shown that the principle of maximal entropy does not always lead to physical states if it is applied to relativistic quantum field theories.
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