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We establish the Alexandroff-Bakelman-Pucci estimate, the Harnack inequality, the H\"older regularity and the Schauder estimates to a class of degenerate parabolic equations of non-divergence form in all dimensions \begin{equation}…

Analysis of PDEs · Mathematics 2024-12-04 Hyo Seok Jang , Ki-Ahm Lee

For any compact connected manifold $M$, we consider the generalized contact Hamiltonian $H(x,p,u)$ defined on $T^*M\times\mathbb R$ which is conex in $p$ and monotonically increasing in $u$. Let $u_\epsilon^-:M\rightarrow\mathbb R$ be the…

Dynamical Systems · Mathematics 2021-06-09 Yanan Wang , Jun Yan , Jianlu Zhang

General Relativity in 4 dimensions can be equivalently described as a dynamical theory of SO(3)-connections rather than metrics. We introduce the notion of asymptotically hyperbolic connections, and work out an analog of the…

General Relativity and Quantum Cosmology · Physics 2017-03-24 Joel Fine , Yannick Herfray , Kirill Krasnov , Carlos Scarinci

For the fifth Painlev\'e equation it is known that a general solution is represented asymptotically by an elliptic function in cheese-like strips near the point at infinity. We present an explicit asymptotic formula for the error term of…

Classical Analysis and ODEs · Mathematics 2025-08-28 Shun Shimomura

In a previous paper we studied the double scaling limit of unitary random matrix ensembles of the form Z_{n,N}^{-1} |\det M|^{2\alpha} e^{-N \Tr V(M)} dM with \alpha > -1/2. The factor |\det M|^{2\alpha} induces critical eigenvalue behavior…

Classical Analysis and ODEs · Mathematics 2015-05-13 A. R. Its , A. B. J. Kuijlaars , J. Ostensson

Definition of generalized normal form for a system of ODEs corresponding to an infinitesimal symplectic or contact transformation near a singular point, with an arbitrary polynomial unperturbed part, and a method of its finding are…

Dynamical Systems · Mathematics 2013-01-15 Arthur S. Vaganyan

A Lam\'e connection is a logarithmic $\mathrm{sl}(2,\mathbb C)$-connection $(E,\nabla)$ over an elliptic curve $X:\{y^2=x(x-1)(x-t)\}$, $t\not=0,1$, having a single pole at infinity. When this connection is irreducible, we show that it is…

Algebraic Geometry · Mathematics 2014-10-21 Frank Loray

We consider the Cauchy problem for the classical Hirota equation on the line with decaying initial data. Based on the spectral analysis of the Lax pair of the Hirota equation, we first expressed the solution of the Cauchy problem in terms…

Mathematical Physics · Physics 2023-01-11 Weikang Xun , Luman Ju , Engui Fan

Rational solutions of the inhomogeneous Painleve-II equation and of a related coupled Painleve-II system have recently arisen in studies of fluid vortices and of the sine-Gordon equation. For the sine-Gordon application in particular it is…

Mathematical Physics · Physics 2013-10-10 Robert J. Buckingham , Peter D. Miller

The necessary and sufficient conditions for a regular positive entire solution $u$ of the biharmonic equation: \begin{equation} \label{0.1} -\Delta^2 u=u^{-p} \;\; \mbox{in $\R^N \; (N \geq 3)$}, \;\; p>1 \end{equation} to be a radially…

Analysis of PDEs · Mathematics 2018-04-24 Zongming Guo , Long Wei , Feng Zhou

We propose a new bilinear Hirota equation for $\tau$-functions associated with the $E_8$ root lattice, that provides a "lens" generalisation of the $\tau$-functions for the elliptic discrete Painlev\'e equation. Our equations are…

Exactly Solvable and Integrable Systems · Physics 2021-02-10 Andrew P. Kels , Masahito Yamazaki

The Painleve-IV equation has three families of rational solutions generated by the generalized Hermite polynomials. Each family is indexed by two positive integers m and n. These functions have applications to nonlinear wave equations,…

Mathematical Physics · Physics 2017-06-29 Robert Buckingham

Gamayun, Iorgov and Lisovyy in 2012 proposed that tau function of the Painlev\'e equation is equal to the series of $c=1$ Virasoro conformal blocks. We study similar series of $c=-2$ conformal blocks and relate it to Painlev\'e theory. The…

Mathematical Physics · Physics 2021-03-08 M. Bershtein , A. Shchechkin

The main subject of the paper is the so-called Discrete Painlev\'e-1 Equation (DP1). Solutions of the DP1 are classified under criterion of their behavior while argument tends to infinity. The appropriate theorems of existence are proved.

High Energy Physics - Theory · Physics 2007-05-23 V. L. Vereschagin

In this paper we present a family of values of the parameters of the third Painlev\'{e} equation such that Puiseux series formally satisfying this equation -- considered as series of $z^{2/3}$ -- are series of exact Gevrey order one. We…

Classical Analysis and ODEs · Mathematics 2017-02-22 Anastasia Parusnikova , Andrey Vasilyev

The paper concerns asymptotic studies for the sixth Painlev\'e transcendent as independent variable tends to infinity. The primary tool is averaging and the Whitham method. Elliptic ansatz, appropriate modulation equation and asymptotics…

Classical Analysis and ODEs · Mathematics 2007-05-23 V. L. Vereschagin

We consider the Clarkson-McLeod solutions of the fourth Painlev\'e equation. This family of solutions behave like $\kappa D_{\alpha-\frac{1}{2}}^2(\sqrt{2}x)$ as $x\rightarrow +\infty$, where $\kappa $ is an arbitrary real constant and…

Mathematical Physics · Physics 2022-04-05 Jun Xia , Shuai-Xia Xu , Yu-Qiu Zhao

We study asymptotically non-free gauge theories and search for renormalization group invariant (i.e. technically natural) relations among the couplings which lead to successful gauge-Yukawa unification. To be definite, we consider a…

High Energy Physics - Theory · Physics 2009-10-28 Jisuke Kubo , Myriam Mondragon , Nicholas D. Tracas , George Zoupanos

Double-pinched Borel-Laplace sum rules are applied to ALEPH $\tau$-decay data. For the leading-twist ($D=0$) Adler function a renormalon-motivated extension is used, and the 5-loop coefficient is taken to be $d_4=275 \pm 63$. Two $D=6$…

High Energy Physics - Phenomenology · Physics 2022-03-01 César Ayala , Gorazd Cvetič , Diego Teca

Two-component hyperbolic system of equations generated by ordinary differential Painlev\'e I \[ u_{yy}=6u^2+y \] and Painlev\'e III \[ yuu_{yy}=yu^2_{y}-uu_y+\delta y+\beta u+\alpha u^3 +\gamma yu^4 \] equations are considered, where…

Exactly Solvable and Integrable Systems · Physics 2016-05-05 O. S. Kostrigina , A. V. Zhiber