@article{8501,
  abstract     = {In this paper, we study small perturbations of a class of non-convex integrable Hamiltonians with two degrees of freedom, and we prove a result of diffusion for an open and dense set of perturbations, with an optimal time of diffusion which grows linearly with respect to the inverse of the size of the perturbation.},
  author       = {Bounemoura, Abed and Kaloshin, Vadim},
  issn         = {1609-3321},
  journal      = {Moscow Mathematical Journal},
  keywords     = {General Mathematics},
  number       = {2},
  pages        = {181--203},
  publisher    = {Independent University of Moscow},
  title        = {{Generic fast diffusion for a class of non-convex Hamiltonians with two degrees of freedom}},
  doi          = {10.17323/1609-4514-2014-14-2-181-203},
  volume       = {14},
  year         = {2014},
}

@article{9166,
  abstract     = {Light-activated self-propelled colloids are synthesized and their active motion is studied using optical microscopy. We propose a versatile route using different photoactive materials, and demonstrate a multiwavelength activation and propulsion. Thanks to the photoelectrochemical properties of two semiconductor materials (α-Fe2O3 and TiO2), a light with an energy higher than the bandgap triggers the reaction of decomposition of hydrogen peroxide and produces a chemical cloud around the particle. It induces a phoretic attraction with neighbouring colloids as well as an osmotic self-propulsion of the particle on the substrate. We use these mechanisms to form colloidal cargos as well as self-propelled particles where the light-activated component is embedded into a dielectric sphere. The particles are self-propelled along a direction otherwise randomized by thermal fluctuations, and exhibit a persistent random walk. For sufficient surface density, the particles spontaneously form ‘living crystals’ which are mobile, break apart and reform. Steering the particle with an external magnetic field, we show that the formation of the dense phase results from the collisions heads-on of the particles. This effect is intrinsically non-equilibrium and a novel principle of organization for systems without detailed balance. Engineering families of particles self-propelled by different wavelength demonstrate a good understanding of both the physics and the chemistry behind the system and points to a general route for designing new families of self-propelled particles.},
  author       = {Palacci, Jérémie A and Sacanna, S. and Kim, S.-H. and Yi, G.-R. and Pine, D. J. and Chaikin, P. M.},
  issn         = {1471-2962},
  journal      = {Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences},
  keywords     = {General Engineering, General Physics and Astronomy, General Mathematics},
  number       = {2029},
  publisher    = {The Royal Society},
  title        = {{Light-activated self-propelled colloids}},
  doi          = {10.1098/rsta.2013.0372},
  volume       = {372},
  year         = {2014},
}

@article{8504,
  abstract     = {In this paper we present a surprising example of a Cr unimodal map of an interval f:I→I whose number of periodic points Pn(f)=∣{x∈I:fnx=x}∣ grows faster than any ahead given sequence along a subsequence nk=3k. This example also shows that ‘non-flatness’ of critical points is necessary for the Martens–de Melo–van Strien theorem [M. Martens, W. de Melo and S. van Strien. Julia–Fatou–Sullivan theory for real one-dimensional dynamics. Acta Math.168(3–4) (1992), 273–318] to hold.},
  author       = {Kaloshin, Vadim and KOZLOVSKI, O. S.},
  issn         = {0143-3857},
  journal      = {Ergodic Theory and Dynamical Systems},
  keywords     = {Applied Mathematics, General Mathematics},
  number       = {1},
  pages        = {159--165},
  publisher    = {Cambridge University Press},
  title        = {{A Cr unimodal map with an arbitrary fast growth of the number of periodic points}},
  doi          = {10.1017/s0143385710000817},
  volume       = {32},
  year         = {2012},
}

@article{8505,
  abstract     = {The classical principle of least action says that orbits of mechanical systems extremize action; an important subclass are those orbits that minimize action. In this paper we utilize this principle along with Aubry-Mather theory to construct (Birkhoff) regions of instability for a certain three-body problem, given by a Hamiltonian system of 2 degrees of freedom. We believe that these methods can be applied to construct instability regions for a variety of Hamiltonian systems with 2 degrees of freedom. The Hamiltonian model we consider describes dynamics of a Sun-Jupiter-comet system, and under some simplifying assumptions, we show the existence of instabilities for the orbit of the comet. In particular, we show that a comet which starts close to an orbit in the shape of an ellipse of eccentricity e=0.66 can increase in eccentricity up to e=0.96. In the sequels to this paper, we extend the result to beyond e=1 and show the existence of ejection orbits. Such orbits are initially well within the range of our solar system. This might give an indication of why most objects rotating around the Sun in our solar system have relatively low eccentricity.},
  author       = {Galante, Joseph and Kaloshin, Vadim},
  issn         = {0012-7094},
  journal      = {Duke Mathematical Journal},
  keywords     = {General Mathematics},
  number       = {2},
  pages        = {275--327},
  publisher    = {Duke University Press},
  title        = {{Destruction of invariant curves in the restricted circular planar three-body problem by using comparison of action}},
  doi          = {10.1215/00127094-1415878},
  volume       = {159},
  year         = {2011},
}

@article{8510,
  abstract     = {In this paper, using the ideas of Bessi and Mather, we present a simple mechanical system exhibiting Arnold diffusion. This system of a particle in a small periodic potential can be also interpreted as ray propagation in a periodic optical medium with a near-constant index of refraction. Arnold diffusion in this context manifests itself as an arbitrary finite change of direction for nearly constant index of refraction.},
  author       = {Kaloshin, Vadim and Levi, Mark},
  issn         = {0273-0979},
  journal      = {Bulletin of the American Mathematical Society},
  keywords     = {Applied Mathematics, General Mathematics},
  number       = {3},
  pages        = {409--427},
  publisher    = {American Mathematical Society},
  title        = {{An example of Arnold diffusion for near-integrable Hamiltonians}},
  doi          = {10.1090/s0273-0979-08-01211-1},
  volume       = {45},
  year         = {2008},
}

@article{8511,
  abstract     = {Here we study an amazing phenomenon discovered by Newhouse [S. Newhouse, Non-density of Axiom A(a) on S2, in: Proc. Sympos. Pure Math., vol. 14, Amer. Math. Soc., 1970, pp. 191–202; S. Newhouse,
Diffeomorphisms with infinitely many sinks, Topology 13 (1974) 9–18; S. Newhouse, The abundance of
wild hyperbolic sets and nonsmooth stable sets of diffeomorphisms, Publ. Math. Inst. Hautes Études Sci.
50 (1979) 101–151]. It turns out that in the space of Cr smooth diffeomorphisms Diffr(M) of a compact
surface M there is an open set U such that a Baire generic diffeomorphism f ∈ U has infinitely many coexisting sinks. In this paper we make a step towards understanding “how often does a surface diffeomorphism
have infinitely many sinks.” Our main result roughly says that with probability one for any positive D a
surface diffeomorphism has only finitely many localized sinks either of cyclicity bounded by D or those
whose period is relatively large compared to its cyclicity. It verifies a particular case of Palis’ Conjecture
saying that even though diffeomorphisms with infinitely many coexisting sinks are Baire generic, they have
probability zero.
One of the key points of the proof is an application of Newton Interpolation Polynomials to study the dynamics initiated in [V. Kaloshin, B. Hunt, A stretched exponential bound on the rate of growth of the number
of periodic points for prevalent diffeomorphisms I, Ann. of Math., in press, 92 pp.; V. Kaloshin, A stretched
exponential bound on the rate of growth of the number of periodic points for prevalent diffeomorphisms II,
preprint, 85 pp.].},
  author       = {Gorodetski, A. and Kaloshin, Vadim},
  issn         = {0001-8708},
  journal      = {Advances in Mathematics},
  keywords     = {General Mathematics},
  number       = {2},
  pages        = {710--797},
  publisher    = {Elsevier},
  title        = {{How often surface diffeomorphisms have infinitely many sinks and hyperbolicity of periodic points near a homoclinic tangency}},
  doi          = {10.1016/j.aim.2006.03.012},
  volume       = {208},
  year         = {2007},
}

@article{8517,
  abstract     = {We consider the evolution of a connected set on the plane carried by a space periodic incompressible stochastic flow. While for almost every realization of the stochastic flow at time t most of the particles are at a distance of order equation image away from the origin, there is a measure zero set of points that escape to infinity at the linear rate. We study the set of points visited by the original set by time t and show that such a set, when scaled down by the factor of t, has a limiting nonrandom shape.},
  author       = {Dolgopyat, Dmitry and Kaloshin, Vadim and Koralov, Leonid},
  issn         = {0010-3640},
  journal      = {Communications on Pure and Applied Mathematics},
  keywords     = {Applied Mathematics, General Mathematics},
  number       = {9},
  pages        = {1127--1158},
  publisher    = {Wiley},
  title        = {{A limit shape theorem for periodic stochastic dispersion}},
  doi          = {10.1002/cpa.20032},
  volume       = {57},
  year         = {2004},
}

@article{8519,
  author       = {Kaloshin, Vadim},
  issn         = {0020-9910},
  journal      = {Inventiones mathematicae},
  keywords     = {General Mathematics},
  number       = {3},
  pages        = {451--512},
  publisher    = {Springer Nature},
  title        = {{The existential Hilbert 16-th problem and an estimate for cyclicity of elementary polycycles}},
  doi          = {10.1007/s00222-002-0244-9},
  volume       = {151},
  year         = {2003},
}

@article{8521,
  abstract     = {We continue the previous article's discussion of bounds, for prevalent diffeomorphisms of smooth compact manifolds, on the growth of the number of periodic points and the decay of their hyperbolicity as a function of their period $n$. In that article we reduced the main results to a problem, for certain families of diffeomorphisms, of bounding the measure of parameter values for which the diffeomorphism has (for a given period $n$) an almost periodic point that is almost nonhyperbolic. We also formulated our results for $1$-dimensional endomorphisms on a compact interval. In this article we describe some of the main techniques involved and outline the rest of the proof. To simplify notation, we concentrate primarily on the $1$-dimensional case.},
  author       = {Kaloshin, Vadim and Hunt, Brian R.},
  issn         = {1079-6762},
  journal      = {Electronic Research Announcements of the American Mathematical Society},
  keywords     = {General Mathematics},
  number       = {5},
  pages        = {28--36},
  publisher    = {American Mathematical Society},
  title        = {{A stretched exponential bound on the rate of growth of the number of periodic points for prevalent diffeomorphisms II}},
  doi          = {10.1090/s1079-6762-01-00091-9},
  volume       = {7},
  year         = {2001},
}

@article{8522,
  abstract     = {For diffeomorphisms of smooth compact manifolds, we consider the problem of how fast the number of periodic points with period $n$grows as a function of $n$. In many familiar cases (e.g., Anosov systems) the growth is exponential, but arbitrarily fast growth is possible; in fact, the first author has shown that arbitrarily fast growth is topologically (Baire) generic for $C^2$ or smoother diffeomorphisms. In the present work we show that, by contrast, for a measure-theoretic notion of genericity we call ``prevalence'', the growth is not much faster than exponential. Specifically, we show that for each $\delta > 0$, there is a prevalent set of ( $C^{1+\rho}$ or smoother) diffeomorphisms for which the number of period $n$ points is bounded above by $\operatorname{exp}(C n^{1+\delta})$ for some $C$ independent of $n$. We also obtain a related bound on the decay of the hyperbolicity of the periodic points as a function of $n$. The contrast between topologically generic and measure-theoretically generic behavior for the growth of the number of periodic points and the decay of their hyperbolicity shows this to be a subtle and complex phenomenon, reminiscent of KAM theory.},
  author       = {Kaloshin, Vadim and Hunt, Brian R.},
  issn         = {1079-6762},
  journal      = {Electronic Research Announcements of the American Mathematical Society},
  keywords     = {General Mathematics},
  number       = {4},
  pages        = {17--27},
  publisher    = {American Mathematical Society},
  title        = {{A stretched exponential bound on the rate of growth of the number of periodic points for prevalent diffeomorphisms I}},
  doi          = {10.1090/s1079-6762-01-00090-7},
  volume       = {7},
  year         = {2001},
}

