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Langevin loops

Fig. 4.22. Comparison between NMF as measured by FCS [46] and simulation using Langevin description [67] with a 2-loop cycle... Fig. 4.22. Comparison between NMF as measured by FCS [46] and simulation using Langevin description [67] with a 2-loop cycle...
The periodicity in the NMF indicates the presence of non-equlibrium processes with periodic solutions and is related to the number of states and the transition rates [46, 67]. It is important to mention that the Langevin simulations are very sensitive to the model used and the identity with the experimental data set is indicative for a driven conformational loop which is coupled to the catalytic step generating the substrate product conversion with photon emission (Fig. 4.22). [Pg.94]

Compared with simulations of the two state model we find perfect agreement. Fitting the time T on the excitation loop as well as the two excitation rates tq and ri to the FHN system, also leads to a reasonable agreement between theory and Langevin simulations of the FHN system. [Pg.63]

The dependence of mean polarization (P3) on the applied electric field in shown in Fig. 4.38a for uniaxial material (Rochelle Salt) parameters, Dirac-delta distribution [T(7 ) = 8(7 — Rq) of particle sizes, fixed freezing radius Rf(T) at temperature 7 = 0 °C and different average nanoparticle radii Rq. Curves 1 for Rq < Rf correspond to Langevin law, while curves 5-7 for Rq > Rf indicate the hysteresis loop appearance. [Pg.274]


See other pages where Langevin loops is mentioned: [Pg.249]    [Pg.249]    [Pg.123]    [Pg.67]    [Pg.125]    [Pg.391]    [Pg.220]    [Pg.65]    [Pg.156]    [Pg.263]    [Pg.275]    [Pg.264]    [Pg.378]    [Pg.244]    [Pg.2098]    [Pg.204]   
See also in sourсe #XX -- [ Pg.231 ]




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