Andrei Sobolevski
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Andrei Sobolevski has a total of 40 co-authors. Here are the top co-authors by number of shared publications:
- Julie Delon
Université Paris Dauphine -PSL Université Paris Dauphine -PSL Université Paris Cité
4 shared publications Julien Salomon
Ceremade
4 shared publications- Eugene Stepanov
St. Petersburg Branch of the Steklov Mathematical Institute of the Russian Academy of Sciences, Fontanka 27, 191023 St. Petersburg, Russia
2 shared publications - Grigory L. Litvinov
NPO Del’fin-Informatika
2 shared publications Konstantin Khanin
Institute for Information Transmission Problems Department of Mathematics Russian Academy of Sciences University of Toronto National Research University Higher School of Economics (HSE)
2 shared publications- Konstantin Khanin
University of Toronto, Toronto, Canada
2 shared publications
Latest Publications
- 1 January 2019
- Published by Tambov State University - G.R. Derzhavin in Russian Universities Reports. Mathematics
- No. 128
Universal algorithms for solving discrete stationary Bellman equations
This paper investigates algorithms for solving discrete stationary (or) matrix Bellman equations over semirings, in particular over tropical and idempotent semirings, Also there are presented some original algorithms, applications and programmed realization.
- 1 January 2019
- Published by Tambov State University - G.R. Derzhavin in Russian Universities Reports. Mathematics
- No. 128
Universal algorithms for solving discrete stationary Bellman equations
This paper investigates algorithms for solving discrete stationary (or) matrix Bellman equations over semirings, in particular over tropical and idempotent semirings, Also there are presented some original algorithms, applications and programmed realization.
- Open Access
Fréchet Barycenters and a Law of Large Numbers for Measures on the Real Line
Endow the space $\mathcal{P}(\mathbb{R})$ of probability measures on $\mathbb{R}$ with a transportation cost $J(\mu, \nu)$ generated by a translation-invariant convex cost function. For a probability distribution on $\mathcal{P}(\mathbb{R})$ we formulate a notion of average with respect to this transportation cost, called here the Fr\'echet barycenter, prove a version of the law of large numbers for Fr\'echet barycenters, and briefly discuss the structure of $\mathcal{P}(\mathbb{R})$ related to the transportation cost $J$.Open AccessFréchet Barycenters and a Law of Large Numbers for Measures on the Real Line
Endow the space $\mathcal{P}(\mathbb{R})$ of probability measures on $\mathbb{R}$ with a transportation cost $J(\mu, \nu)$ generated by a translation-invariant convex cost function. For a probability distribution on $\mathcal{P}(\mathbb{R})$ we formulate a notion of average with respect to this transportation cost, called here the Fr\'echet barycenter, prove a version of the law of large numbers for Fr\'echet barycenters, and briefly discuss the structure of $\mathcal{P}(\mathbb{R})$ related to the transportation cost $J$. - Open Access
- 25 August 2015
- Published by SAGE Publications in Perception
- Vol. 44 (8-9) , 837-850
Scientific Activity of Alfred Yarbus: The Stages of Research Work, Senior and Younger Colleagues, Conditions of Investigations
- 25 August 2015
- Published by SAGE Publications in Perception
- Vol. 44 (8-9) , 837-850
Open AccessScientific Activity of Alfred Yarbus: The Stages of Research Work, Senior and Younger Colleagues, Conditions of Investigations
- 15 August 2015
- Published by Springer Nature in Archive for Rational Mechanics and Analysis
- Vol. 219 (2) , 861-885
On Dynamics of Lagrangian Trajectories for Hamilton–Jacobi Equations
- 15 August 2015
- Published by Springer Nature in Archive for Rational Mechanics and Analysis
- Vol. 219 (2) , 861-885
On Dynamics of Lagrangian Trajectories for Hamilton–Jacobi Equations
- Open Access
On dynamics of Lagrangian trajectories for Hamilton-Jacobi equations
Characteristic curves of a Hamilton-Jacobi equation can be seen as action minimizing trajectories of fluid particles. However this description is valid only for smooth solutions. For nonsmooth "viscosity" solutions, which give rise to discontinuous velocity fields, this picture holds only up to the moment when trajectories hit a shock and cease to minimize the Lagrangian action. In this paper we discuss two physically meaningful regularisation procedures, one corresponding to vanishing viscosity and another to weak noise limit. We show that for any convex Hamiltonian, a viscous regularization allows to construct a nonsmooth flow that extends particle trajectories and determines dynamics inside the shock manifolds. This flow consists of integral curves of a particular "effective" velocity field, which is uniquely defined everywhere in the flow domain and is discontinuous on shock manifolds. The effective velocity field arising in the weak noise limit is generally non-unique and different from the viscous one, but in both cases there is a fundamental self-consistency condition constraining the dynamics.
Open AccessOn dynamics of Lagrangian trajectories for Hamilton-Jacobi equations
Characteristic curves of a Hamilton-Jacobi equation can be seen as action minimizing trajectories of fluid particles. However this description is valid only for smooth solutions. For nonsmooth "viscosity" solutions, which give rise to discontinuous velocity fields, this picture holds only up to the moment when trajectories hit a shock and cease to minimize the Lagrangian action. In this paper we discuss two physically meaningful regularisation procedures, one corresponding to vanishing viscosity and another to weak noise limit. We show that for any convex Hamiltonian, a viscous regularization allows to construct a nonsmooth flow that extends particle trajectories and determines dynamics inside the shock manifolds. This flow consists of integral curves of a particular "effective" velocity field, which is uniquely defined everywhere in the flow domain and is discontinuous on shock manifolds. The effective velocity field arising in the weak noise limit is generally non-unique and different from the viscous one, but in both cases there is a fundamental self-consistency condition constraining the dynamics.
- Open Access
- 16 April 2013
- Published by Mathematical Sciences Publishers in Pacific Journal of Mathematics
- Vol. 262 (2) , 457-480
Droplet condensation and isoperimetric towers
We consider a variational problem in a planar convex domain, motivated by statistical mechanics of crystal growth in a saturated solution. The minimizers are constructed explicitly and are completely characterized
- 16 April 2013
- Published by Mathematical Sciences Publishers in Pacific Journal of Mathematics
- Vol. 262 (2) , 457-480
Open AccessDroplet condensation and isoperimetric towers
We consider a variational problem in a planar convex domain, motivated by statistical mechanics of crystal growth in a saturated solution. The minimizers are constructed explicitly and are completely characterized
- 26 March 2013
- Published by Springer Nature in Soft Computing
- Vol. 17 (10) , 1767-1785
Universal algorithms for solving the matrix Bellman equations over semirings
- 26 March 2013
- Published by Springer Nature in Soft Computing
- Vol. 17 (10) , 1767-1785
Universal algorithms for solving the matrix Bellman equations over semirings
- Open Access
Droplet condensation and isoperimetric towers
We consider a variational problem in a planar convex domain, motivated by statistical mechanics of crystal growth in a saturated solution. The minimizers are constructed explicitly and are completely characterized.
Open AccessDroplet condensation and isoperimetric towers
We consider a variational problem in a planar convex domain, motivated by statistical mechanics of crystal growth in a saturated solution. The minimizers are constructed explicitly and are completely characterized.
- 4 January 2013
- Published by American Physical Society (APS) in Physical Review E
- Vol. 87 (1) , 012102
Planar diagrams from optimization for concave potentials
We propose a toy model of a heteropolymer chain capable of forming planar secondary structures typical for RNA molecules. In this model, the sequential intervals between neighboring monomers along a chain are considered as quenched random variables, and energies of nonlocal bonds are assumed to be concave functions of those intervals. A few factors are neglected: the contribution of loop factors to the partition function, the variation in energies of different types of complementary nucleotides, the stacking interactions, and constraints on the minimal size of loops. However, the model captures well the formation of folded structures without pseudoknots in an arbitrary sequence of nucleotides. Using the optimization procedure for a special class of concave-type potentials, borrowed from optimal transport analysis, we derive the local difference equation for the ground state free energy of the chain with the planar (RNA-like) architecture of paired links. We consider various distribution functions of intervals between neighboring monomers (truncated Gaussian and scale free) and demonstrate the existence of a topological crossover from sequential to essentially nested configurations of paired links.
- 4 January 2013
- Published by American Physical Society (APS) in Physical Review E
- Vol. 87 (1) , 012102
Planar diagrams from optimization for concave potentials
We propose a toy model of a heteropolymer chain capable of forming planar secondary structures typical for RNA molecules. In this model, the sequential intervals between neighboring monomers along a chain are considered as quenched random variables, and energies of nonlocal bonds are assumed to be concave functions of those intervals. A few factors are neglected: the contribution of loop factors to the partition function, the variation in energies of different types of complementary nucleotides, the stacking interactions, and constraints on the minimal size of loops. However, the model captures well the formation of folded structures without pseudoknots in an arbitrary sequence of nucleotides. Using the optimization procedure for a special class of concave-type potentials, borrowed from optimal transport analysis, we derive the local difference equation for the ground state free energy of the chain with the planar (RNA-like) architecture of paired links. We consider various distribution functions of intervals between neighboring monomers (truncated Gaussian and scale free) and demonstrate the existence of a topological crossover from sequential to essentially nested configurations of paired links.
- 2 March 2012
- Published by Springer Nature in Journal of Mathematical Sciences
- Vol. 181 (6) , 782-791
Minimum—weight perfect matching for nonintrinsic distances on the line
- 2 March 2012
- Published by Springer Nature in Journal of Mathematical Sciences
- Vol. 181 (6) , 782-791
Minimum—weight perfect matching for nonintrinsic distances on the line