1957
DOI: 10.1143/jpsj.12.1203
|View full text |Cite
|
Sign up to set email alerts
|

Statistical-Mechanical Theory of Irreversible Processes. II. Response to Thermal Disturbance

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

4
439
1
1

Year Published

1963
1963
2017
2017

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 726 publications
(445 citation statements)
references
References 6 publications
4
439
1
1
Order By: Relevance
“…There simply is no external field which could exert a force on heat, heat is always driven by an energy density (temperature) gradient as described by (1b). Nevertheless, as will also be sketched below, there have been attempts to apply the derivation of (1a) to thermal conduction which eventually implies the application of the KF also in this case 1,2,3,4 . Let us briefly recall the derivation of the KF.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…There simply is no external field which could exert a force on heat, heat is always driven by an energy density (temperature) gradient as described by (1b). Nevertheless, as will also be sketched below, there have been attempts to apply the derivation of (1a) to thermal conduction which eventually implies the application of the KF also in this case 1,2,3,4 . Let us briefly recall the derivation of the KF.…”
Section: Introductionmentioning
confidence: 99%
“…dτ Tr{ρ 0ĵ (0)ĵ(t + iτ )}, (2) whereρ 0 is the Gibbsian equilibrium state, V the volume and L(ω) is the response coefficient which describes the conductivity at frequency ω.…”
Section: Introductionmentioning
confidence: 99%
“…We come to our main result that generalizes the classical result of Green 1 and Kubo 2,3 for Hamiltonian systems to nonHamiltonian systems of the form ͑1͒.…”
Section: A Green-kubo Relationsmentioning
confidence: 67%
“…There are few possible ways for taking such perturbations into account. The response of a weakly nonequilibrium system on a thermal type perturbation can be represented as a Fourier transforms of the time correlation functions of the operators for corresponding flows with statistically equilibrium system state [48]. The admittances of this type structure is similar to the expressions for kinetic coefficients, emerging in the equilibrium systems theory as a reaction on mechanical type perturbation, which are representable in the form of an additional summand in the Hamiltonian of the system.…”
Section: Introductionmentioning
confidence: 99%