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We prove a Fredholm determinant and short-distance series representation of the Painlev\'e V tau function $\tau(t)$ associated to generic monodromy data. Using a relation of $\tau(t)$ to two different types of irregular $c=1$ Virasoro…

Mathematical Physics · Physics 2018-10-10 O. Lisovyy , H. Nagoya , J. Roussillon

We evaluate explicitly, in terms of the Cauchy data, the constant pre-factor in the large $x$ asymptotics of the Painlev\'e III tau-function. Our result proves the conjectural formula for this pre-factor obtained recently by O. Lisovyy, Y.…

Mathematical Physics · Physics 2018-02-01 Alexander Its , Andrei Prokhorov

Generic c=1 four-point conformal blocks on the Riemann sphere can be seen as the coefficients of Fourier expansion of the tau function of Painlev\'e VI equation with respect to one of its integration constants. Based on this relation, we…

High Energy Physics - Theory · Physics 2013-12-19 N. Iorgov , O. Lisovyy , Yu. Tykhyy

We examine the two-point correlation functions of the fields exp(i$\alpha\Phi$) in the sine-Gordon theory at all values of the coupling constant $\hat\beta$. Using conformal perturbation theory, we write down explicit integral expressions…

High Energy Physics - Theory · Physics 2016-09-06 Robert M. Konik , Andre LeClair

We propose a relation the expansions of regular and irregular semiclassical conformal blocks at different branch points making use of the connection between the accessory parameters of the BPZ decoupling equations to the logarithm…

High Energy Physics - Theory · Physics 2024-08-26 Bruno Carneiro da Cunha , João Paulo Cavalcante

We prove a conjecture on uniqueness and existence of the irregular vertex operators of rank $r$ introduced in our previous paper. We also introduce ramified irregular vertex operators of the Virasoro algebra. As applications, we give…

Mathematical Physics · Physics 2018-11-09 Hajime Nagoya

We reformulate the $q$-difference linear system corresponding to the $q$-Painlev\'e equation of type $A_7^{(1)'}$ as a Riemann-Hilbert problem on a circle. Then, we consider the Fredholm determinant built from the jump of this…

Mathematical Physics · Physics 2025-01-03 Pavlo Gavrylenko

This paper is based on my presentation at RIMS workshop on "Theory of Integrable Systems and Its Applications in Various Fields" held in Kyoto on 19--21, August 2015. The aim of the present paper is to give a short account of recent studies…

Mathematical Physics · Physics 2016-11-29 Hajime Nagoya

The connection problem for isomonodromic tau functions on the one-punctured torus concerns the ratio between the tau function and its modular transform, associated to dual pants decompositions of the torus. In this paper, we study the…

Mathematical Physics · Physics 2025-08-20 Fabrizio Del Monte , Harini Desiraju , Pavlo Gavrylenko

We prove that the tau-function of the integrable discrete sine-Gordon model apart from the "standard" bilinar identities obeys a number of "non-standard" ones. They can be combined into a bivector 3-dimensional difference equation which is…

solv-int · Physics 2007-05-23 A. Zabrodin

We study the dependence of the tau function of Painlev\'e I equation on the generalized monodromy of the associated linear problem. In particular, we compute connection constants relating the tau function asymptotics on five canonical rays…

Exactly Solvable and Integrable Systems · Physics 2017-05-30 O. Lisovyy , J. Roussillon

Generic Painlev\'e VI tau function \tau(t) can be interpreted as four-point correlator of primary fields of arbitrary dimensions in 2D CFT with c=1. Using AGT combinatorial representation of conformal blocks and determining the…

High Energy Physics - Theory · Physics 2013-12-19 O. Gamayun , N. Iorgov , O. Lisovyy

We elucidate the relation between Painlev\'e equations and four-dimensional rank one ${\cal N= 2}$ theories by identifying the connection associated to Painlev\'e isomonodromic problems with the oper limit of the flat connection of the…

High Energy Physics - Theory · Physics 2017-09-20 Giulio Bonelli , Oleg Lisovyy , Kazunobu Maruyoshi , Antonio Sciarappa , Alessandro Tanzini

We discuss an extension of the Jimbo-Miwa-Ueno differential 1-form to a form closed on the full space of extended monodromy data of systems of linear ordinary differential equations with rational coefficients. This extension is based on the…

Mathematical Physics · Physics 2018-10-30 A. Its , O. Lisovyy , A. Prokhorov

We study the relation of irregular conformal blocks with the Painlev\'e III$_3$ equation. The functional representation for the quasiclassical irregular block is shown to be consistent with the BPZ equations of conformal field theory and…

Mathematical Physics · Physics 2021-02-03 Pavlo Gavrylenko , Andrei Marshakov , Artem Stoyan

The goal of this note is to show that the Riemann-Hilbert problem to find multivalued analytic functions with $SL(2,\mathbb{C})$-valued monodromy on Riemann surfaces of genus zero with $n$ punctures can be solved by taking suitable linear…

High Energy Physics - Theory · Physics 2016-04-15 N. Iorgov , O. Lisovyy , J. Teschner

We introduce the tau-function of a rational d-connection and its isomonodromy transformations. We show that in a continuous limit our tau-function agrees with the Jimbo-Miwa-Ueno tau-function, compute the tau-function for the isomonodromy…

Algebraic Geometry · Mathematics 2014-01-14 D. Arinkin , A. Borodin

We determine the strong coupling constant \alpha_s from the \tau hadroni width using a renormalization group summed (RGS) expansion of the QCD Adler function. The main theoretical uncertainty in the extraction of \alpha_s is due to the…

High Energy Physics - Phenomenology · Physics 2015-06-16 Gauhar Abbas , B. Ananthanarayan , I. Caprini

Classical conformal blocks naturally appear in the large central charge limit of 2D Virasoro conformal blocks. In the $AdS_{3}/CFT_{2}$ correspondence, they are related to classical bulk actions and are used to calculate entanglement…

High Energy Physics - Theory · Physics 2018-05-10 Máté Lencsés , Fábio Novaes

The degenerate third Painlev\'{e} equation, $u^{\prime \prime} = \frac{(u^{\prime})^{2}}{u} - \frac{u^{\prime}}{\tau} + \frac{1}{\tau}(-8 \epsilon u^{2} + 2ab) + \frac{b^{2}}{u}$, where $\epsilon,b \in \mathbb{R}$, and $a \in \mathbb{C}$,…

Classical Analysis and ODEs · Mathematics 2009-11-10 A. V. Kitaev , A. H. Vartanian
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