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Fluctuation-dissipation theorem variance

As mentioned, this equivalence is a consequence of the fluctuation-dissipation theorem (the general basis of linear response theory [51]). In (12.68), we have dropped nonlinear terms and we have not indicated for which state Variance (rj) is computed (because the reactant and product state results only differ by nonlinear terms). We see that A A, AAstat, and AAr x are all linked and are all sensitive to the model parameters, with different computational routes giving a different sensitivity for AArtx. [Pg.453]

With regard to the microcanonical equilibrium distribution and the extension of the fluctuation-dissipation theorem, we considered a nonergodic adiabatic invariant in a simple Hamiltonian chaotic system. We numerically demonstrated the breaking of the nonergodic adiabatic invariant in the mixed phase space. The variance of the nonergodic adiabatic invariant can be considered as a measure for complexity of the mixed phase space. [Pg.368]


See other pages where Fluctuation-dissipation theorem variance is mentioned: [Pg.325]    [Pg.245]    [Pg.202]    [Pg.277]   
See also in sourсe #XX -- [ Pg.361 , Pg.362 , Pg.363 , Pg.364 , Pg.365 , Pg.366 , Pg.367 ]

See also in sourсe #XX -- [ Pg.361 , Pg.362 , Pg.363 , Pg.364 , Pg.365 , Pg.366 , Pg.367 ]




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