Christian Beck, Friedrich Schögl · Cambridge University Press eBooks · 1993
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Beck, C. · RWTH Publications (RWTH Aachen) · 1995
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Christian Beck · Physica D Nonlinear Phenomena · 1995
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Harm Bart · Linear Algebra and its Applications · 1986
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Selberg Zeta Function, Arash Momeni, Alexei Venkov · 2010
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Mark Pollicott · Journal of Statistical Physics · 2016
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Adam Nielsen, Konstantin Fackeldey, Marcus Weber · 2013
We introduce a generalized operator for arbitrary stochastic processes by using a pre-kernel, which is a generalization of the Markov kernel. For deterministic processes, such an operator is already known as the Frobenius-Perron operator, which is defined for a large class of measures. For Markov processes, there exists transfer operators being only well defined for stationary measures in $L^2$. Our novel generalized transfer operator is well defined for arbitrary stochastic processes, in particular also for deterministic ones. We can show that this operator is acting on $L^1$. For stationary measures, this operator is also an endomorphism of $L^2$ and, therefore, allows for a mathematical analysis in Hilbert spaces.
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2015
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2017
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TUScholarShare (Temple University) · 1948
John Rycerz, trolley operator, is seen in profile, scratching his head and holding stacks of transfer and rebate slips.
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Zaitsev, Oleg, Narevich, R., Prange, R. E. · arXiv (Cornell University) · 1999
The trace formulas commonly used in discussing spectral properties of quantum or wave systems are derived simply and directly from the Bogomolny transfer operator. Special cases are the Gutzwiller formula, the Berry-Tabor formula, and the perturbed Berry-Tabor formula. A comment is made about interpolation formulas proposed in the latter case.
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D. A. Goodings, N. D. Whelan · 1998
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Garcia-Vidal, Francisco J., Feist, Johannes · Biblos-e Archivo (Universidad Autónoma de Madrid) · 2019
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F. J. Garcı́a-Vidal, Johannes Feist · Science · 2017
Nanophotonics can be used to enhance the electromagnetic coupling between molecules
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Thomas Prellberg · 2003
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Lev Sakhnovich · Birkhäuser Basel eBooks · 1999
Consider a dynamical system of the form 0.1 $$ \frac{{dx}}{{dt}} = Ax + I{I_1}v,y = {\Gamma _2}^*x + {v_1}$$ where v(t) and y(t) are functions taking values in a Hilbert space $$\mathfrak{G}$$ , and x(t) is a function taking values in a Hilbert space $$\mathfrak{H}$$ .
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Christof Schà ⁄ tte, Marco Sarich · Courant lecture notes in mathematics · 2013
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R. E. Prange, Олег Зайцев, R. Narevich · Physica E Low-dimensional Systems and Nanostructures · 2001
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CUHK Digital Repository (Chinese University of Hong Kong) · 2011
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Stéphane Descombes, Boun Oumar Dia · Journal of Functional Analysis · 1999
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