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Titlebook: Dynamical Systems and Microphysics; A. Blaquiére,F. Fer,A. Marzollo Book 1980 Springer-Verlag Wien 1980 Systems.dynamical system.dynamical

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樓主: Randomized
41#
發(fā)表于 2025-3-28 17:54:57 | 只看該作者
https://doi.org/10.1007/978-3-662-64178-1 at the microscopic scale. Any evolution of the mean behaviour of such collective processes is characterized by two very important effects: the existence of fluctuations and the appearance of irreversibility. Indeed, the latter never occurs in the dynamic laws governing the trajectories of only a ve
42#
發(fā)表于 2025-3-28 21:04:01 | 只看該作者
Wahn und Wahnsinn im Stummfilm,cesses. This problem has been the object of many attempts. It is generally accepted that probabilistic processes can arise from deterministic dynamics through a process of “coarse-graining”, “contraction of the description” or by introducing extra dynamic approximations like the “molecular chaos”. I
43#
發(fā)表于 2025-3-29 02:25:25 | 只看該作者
44#
發(fā)表于 2025-3-29 03:27:23 | 只看該作者
Kinematics and Dynamics of It? Processes “position variable” q(t) ∈ R. must be interpreted as a continuous Markov process described by the stochastic differential equation . with initial condition q(0)=q., h being the Planck’s constant, m the mass of the particle and w(t) the standard Brownian motion.
45#
發(fā)表于 2025-3-29 10:02:52 | 只看該作者
46#
發(fā)表于 2025-3-29 11:31:50 | 只看該作者
Stochastic Electrodynamics: Methods and Results of a universal stochastic electromagnetic field (“background” field or “zero-point” field), which could be conceived as a classical counterpart to the vacuum field of Quantum Electrodynamics (QED). Thus this stochastic field (uniform and isotropic) has zero mean and spectral density [1–4].
47#
發(fā)表于 2025-3-29 17:29:21 | 只看該作者
48#
發(fā)表于 2025-3-29 22:24:54 | 只看該作者
Dynamical Systems and Microphysics978-3-7091-4330-8Series ISSN 0254-1971 Series E-ISSN 2309-3706
49#
發(fā)表于 2025-3-30 03:24:52 | 只看該作者
50#
發(fā)表于 2025-3-30 06:43:45 | 只看該作者
https://doi.org/10.1007/978-3-662-63550-6 “position variable” q(t) ∈ R. must be interpreted as a continuous Markov process described by the stochastic differential equation . with initial condition q(0)=q., h being the Planck’s constant, m the mass of the particle and w(t) the standard Brownian motion.
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