2008
DOI: 10.1070/rm2008v063n01abeh004500
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Reversibility and irreversibility in stochastic chemical kinetics

Abstract: Mathematical problems with mean field and local type interaction related to stochastic chemical kinetics,are considered˙Our main concern various definitions of reversibility, their corollaries (Boltzmann type equations, fluctuations,Onsager relations, etc) and emergence of irreversibility.

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Cited by 18 publications
(13 citation statements)
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“…It also differs from those focusing on moments (Gadgil et al, 2006) but leans towards those of nonequilibrium thermodynamics approaches (Qian, 2005). In addition, it differs from other more formal stochastic approaches in biology but more from a mathematical point of view (Malyshev and Pirogov, 2008). The powerful adaptive landscape concept was first proposed by a great biologist a long time ago (Wright, 1932).…”
Section: Introductionmentioning
confidence: 99%
“…It also differs from those focusing on moments (Gadgil et al, 2006) but leans towards those of nonequilibrium thermodynamics approaches (Qian, 2005). In addition, it differs from other more formal stochastic approaches in biology but more from a mathematical point of view (Malyshev and Pirogov, 2008). The powerful adaptive landscape concept was first proposed by a great biologist a long time ago (Wright, 1932).…”
Section: Introductionmentioning
confidence: 99%
“…The equations for complex physicochemical processes in the general form are written as [6,7,11,12,24,25]:…”
Section: The Methods and Definitionsmentioning
confidence: 99%
“…The first of them formulates the conservation law of the number of atoms (or complexes of atoms) of the form A: N 1 +N 3 , the second one is the number of atoms of the form B, the second one is the number of atoms of the form B: N 2 + N 3 , and the third law is the number of atoms of the form C: N 2 + N 4 . It is easy to verify that a linear operator: I µ (t) = n i=1 µ i N i (t) = (µ, N) is conserved along the solutions of the system under consideration then and only then when the vector µ is orthogonal to all Boltzmann-Orlov-Moser-Bruno vectors [12,[24][25][26][27] α − β. In this example, the Boltzmann-Orlov-Moser-Bruno vector is unique up to a factor: α − β = (1, 1, −1, −1).…”
Section: The Methods and Definitionsmentioning
confidence: 99%
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“…4. Проверить, что во всех этих случаях пределы временных средних совпадают с экстремалями Больцмана, обобщая и упрощая результаты работ [1]- [28].…”
Section: Introductionunclassified