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- 10189_2017_Article_160247@epje160247. dvi - Springer
The model consists of a Langevin equation of the form dv v m = −μ N + ξ(t), dt v | | left-hand side of eq (1) but in both cases solid friction and noise play the dominant role ) The most realistic physical realization of eq (1) is the two-dimensional system, where the particle is placed on a vibrating plane
- Journal Club - Karger Publishers
Bell IR, Howerter A, Jackson N, Aickin M, Bootzin RR, Brooks AJ: Nonlinear dynamical systems effects of homeopathic remedies on multiscale entropy and correlation dimension of slow wave sleep EEG in young adults with histories of coffee-induced insomnia
- RESEARCH ARTICLE Open Access Short term in-patient . . .
Short term in-patient rehabilitation in axial spondyloarthritis - the results of a 2-week program performed in daily clinical practice Siv Grødal Eppeland1, Andreas P Diamantopoulos1,2, Dag Magnar Soldal1 and Glenn Haugeberg1,2*
- Stochastic rolling of a rigid sphere in weak adhesive contact . . .
Stochastic rolling of a rigid sphere in weak adhesive contact with a soft substrate P S Goohpattader, S Mettu, and M K Chaudhurya
- Exploration of sub-bandgap states in 2D halide perovskite . . .
2(CH 3HN 3)n−1MnX 3n+1,whereRisan organic moiety, M is a divalent cation, X is single or a mixture of halide anions, and n is the number of [MX 6] 4−sheets between organic layers5 The
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