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Generative models of cell dynamics: from Neural ODEs to flow matching. [PDF]
Richter T, Wang W, Palma A, Theis FJ.
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Class of Perturbation Theories of Ordinary Differential Equations
Journal of Mathematical Physics, 1971A class of perturbation theories of ordinary differential equations is studied in a systematic and rigorous way. This class contains the perturbation theory by Kruskal [J. Math. Phys. 3, 806 (1962)] and its generalization discussed by Coffey [J. Math. Phys.
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Regular Perturbation of Ordinary Differential Equations
2015In this chapter we find asymptotic solutions of regularly perturbed equations and systems of equations, to which problems in mechanics are reduced. We consider Cauchy problems, problems for periodic solutions and boundary value problems.
S. M. Bauer +4 more
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Perturbations of Multipliers of Systems of Periodic Ordinary Differential Equations
Advances in Applied Mathematics and Mechanics, 2011AbstractThe paper deals with periodic systems of ordinary differential equations (ODEs). A new approach to the investigation of variations of multipliers under perturbations is suggested. It enables us to establish explicit conditions for the stability and instability of perturbed systems.
Leonid Berezansky +2 more
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Lie equations for asymptotic solutions of perturbation problems of ordinary differential equations
Journal of Mathematical Physics, 2009Lie theory is applied to perturbation problems of ordinary differential equations to construct approximate solutions and invariant manifolds according to the renormalization group approach of Iwasa and Nozaki [“A method to construct asymptotic solutions invariant under the renormalization group,” Prog. Theor. Phys. 116, 605 (2006)].
Chiba, Hayato, Iwasa, Masatomo
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Journal of Mathematical Sciences, 2020
Consider a system of differential equations \[ \varphi^{(1)}=\omega,\ \ \varepsilon a(\varphi)x^{(n+1)}+x^{(n)}+b_{1}(\varphi)x^{(n-1)}+\ldots+b_{n}(\varphi)x=f(\varphi),\tag{1} \] where \(\varphi \in \mathbb R^{m}\), \(\omega =(\omega_{1},\omega_{2},\ldots,\omega_{m})\) is a frequence basis, \(x\in \mathbb R\), \(f\in \mathcal T^{m}\) and \(\mathcal T^
Er'omenko, V. O., Aliluiko, A. M.
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Consider a system of differential equations \[ \varphi^{(1)}=\omega,\ \ \varepsilon a(\varphi)x^{(n+1)}+x^{(n)}+b_{1}(\varphi)x^{(n-1)}+\ldots+b_{n}(\varphi)x=f(\varphi),\tag{1} \] where \(\varphi \in \mathbb R^{m}\), \(\omega =(\omega_{1},\omega_{2},\ldots,\omega_{m})\) is a frequence basis, \(x\in \mathbb R\), \(f\in \mathcal T^{m}\) and \(\mathcal T^
Er'omenko, V. O., Aliluiko, A. M.
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Non-standard analysis and singular perturbations of ordinary differential equations
Russian Mathematical Surveys, 1984This is a lively and interesting survey of a lively and interesting area of current research, namely the application of non-standard analysis to singular perturbation problems for ordinary differential equations. In particular, the authors discuss certain singular solutions (called ''ducks'') of nonlinear second-order equations depending on a small ...
Zvonkin, A. K., Shubin, M. A.
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Invariant manifolds of singularly perturbed ordinary differential equations
ZAMP Zeitschrift f�r angewandte Mathematik und Physik, 1985Consider an autonomous system \[ (1)\quad dx/dt=f(x,y,\epsilon),\quad \epsilon dy/dt=g(x,y,\epsilon), \] where \(f: D\to {\mathbb{R}}^ m\), \(g: D\to {\mathbb{R}}^ n\), \(D=D_ 1\times D_ 2\times (-\epsilon_ 0,\epsilon_ 0)\) is a bounded domain in \({\mathbb{R}}^{m+n+1}\), and \(D_ 1\) is star shaped with \(C^{\nu +1}\) boundary, \(\nu\geq 1\).
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