Download Cumulative Author, Title and Subject Index Including Table by C. Domb and J.L. Lebowitz (Eds.) PDF

By C. Domb and J.L. Lebowitz (Eds.)

The sphere of section transitions and important phenomena is still lively in learn, generating a gentle flow of fascinating and fruitful effects. It has moved right into a primary position in condensed topic reports. Statistical physics, and extra particularly, the speculation of transitions among states of subject, kind of defines what we all know approximately 'everyday' subject and its adjustments. the main objective of this serial is to supply assessment articles that may function typical references for learn staff within the box, and for graduate scholars and others wishing to acquire trustworthy details on vital fresh advancements.

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Read or Download Cumulative Author, Title and Subject Index Including Table of Contents, Volumes 1–19 PDF

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Extra info for Cumulative Author, Title and Subject Index Including Table of Contents, Volumes 1–19

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121) is called the generalized Langevin equation or the Mori–Zwanzig equation. 107). A special situation occurs in the case of stationarity. 7 Stochastic Equations of Motion 41 ˆ α (t − t )) = − (fβ (t ) , fα (t)), which where we have used the relation (G0β , Lf can be checked straightforwardly. For the sake of simplicity, we set t0 = 0. Then, due to the stationarity, we obtain ˆ LG ˆ 0 , fα (t − t )). 125) ˆ β (t ) , fα (t)). 108), which is valid, of course, for all dynamic quantities of the system.

97) may be specified for the case where the state space consists of discrete numbers only. 99) ∂t m with Wnm (t) = W (n | m; t) and pnm (t, t ) = p (n, t | m, t ). In this representation, the concept of jump processes becomes particularly clear. But it should be noted again that pure jump processes can occur even in a continuous state space1 . ). 55), all conditional probabilities are also invariant under a time shift. 85) are simple functions of 1 Of course, the trajectory of a large but finite complex system has no real jumps.

41) with L ˆ 1 by Q ˆL ˆ and L ˆ 2 by by a derivative with respect to the time. If we replace L ˆ we arrive at Pˆ L, ˆ ˆˆ ˆ LG ˆ 0α = eQL(t−t0 ) Q ˆ LG ˆ 0α eL(t−t0 ) Q t ˆ QL(t −t0 ) Q ˆ LG ˆ 0α . 117) 40 2. 33), the first contribution can be transformed into ˆˆ ˆˆ ˆ QL(t−t0 ) Q ˆ LG ˆ 0α = Qe ˆ LG ˆ 0α . 118) This quantity is referred to as the fluctuating force or the residual force. By ˆ LG ˆ 0 is ruled construction, the time evolution of fα (t) from its initial value Q α ˆ ˆ by the anomalous propagator exp{QL(t − t0 )} rather than by the usual one, ˆ − t0 )}.

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