From the KP hierarchy to the Painlevé equations

Slides:



Advertisements
Similar presentations
Solve a System Algebraically
Advertisements

Backlund Transformations for Non-Commutative (NC) Integrable Eqs. Masashi HAMANAKA University of Nagoya (visiting Glasgow until Feb. 13 and IHES Feb13.
Gravitational and electromagnetic solitons Monodromy transform approach Solution of the characteristic initial value problem; Colliding gravitational and.
Algebra Recap Solve the following equations (i) 3x + 7 = x (ii) 3x + 1 = 5x – 13 (iii) 3(5x – 2) = 4(3x + 6) (iv) 3(2x + 1) = 2x + 11 (v) 2(x + 2)
Chapter 2: Second-Order Differential Equations
Solving Equations = 4x – 5(6x – 10) -132 = 4x – 30x = -26x = -26x 7 = x.
PERTURBED NONLINEAR EVOLUTION EQUATIONS AND ASYMPTOTIC INTEGRABILITY Yair Zarmi Physics Department & Jacob Blaustein Institutes for Desert Research Ben-Gurion.
Stanford University Department of Aeronautics and Astronautics Introduction to Symmetry Analysis Brian Cantwell Department of Aeronautics and Astronautics.
Inverse Problems in Semiconductor Devices Martin Burger Johannes Kepler Universität Linz.
1 Section 2 SECTION 2 Partial Fractions. 2 We need to split the following into separate terms: Roots of the denominator D(s): Case I – unrepeated factor.
A Backlund Transformation for Noncommutative Anti-Self-Dual Yang-Mills (ASDYM) Equations Masashi HAMANAKA University of Nagoya, Dept. of Math. LMS Durham.
Jeopardy comments/answers April Existence Uniqueness Each kind of differential equation we studied had a corresponding existence and uniqueness.
Noncommutative Solitons and Integrable Systems  MH,``Conservation laws for NC Lax hierarchy, ’’ JMP46(2005)052701[hep-th/ ]  MH, ``NC Ward's conjecture.
Inverse Kinematics Problem: Input: the desired position and orientation of the tool Output: the set of joints parameters.
Noncommutative Solitons and Integrable Systems Masashi HAMANAKA University of Nagoya, Dept. of Math. Based on  C.R.Gilson (Glasgow), MH and J.J.C.Nimmo.
Systems of Equations and Inequalities in Two Variables A-REI.3; A-REI.5; A-REI.6; A-REI.7.
1 Part 1: Ordinary Differential Equations Ch1: First-Order Differential Equations Ch2: Second-Order Differential Equations Ch3: The Laplace Transform Ch4:
Chapter 3: The Laplace Transform
Noncommutative Integrable Systems and Quasideterminants. Masashi HAMANAKA University of Nagoya, Dept of Math. Based on Claire R.Gilson (Glasgow), MH and.
II. System of Non-Homogeneous Linear Equations Coefficient Matrix Matrix form Of equations Guiding system (1)(1)
Jeffrey D. Tare* and Jose Perico H. Esguerra
Math 3120 Differential Equations with Boundary Value Problems
1 Part II: Linear Algebra Chapter 8 Systems of Linear Algebraic Equations; Gauss Elimination 8.1 Introduction There are many applications in science and.
String solitons in the M5-brane worldvolume with a Nambu-Poisson structure and Seiberg-Witten map Tomohisa Takimi (NTU) Ref ) Kazuyuki Furuuchi, T.T JHEP08(2009)050.
D-term Dynamical Supersymmetry Breaking K. Fujiwara and, H.I. and M. Sakaguchi arXiv: hep-th/ , P. T. P. 113 arXiv: hep-th/ , N. P. B 723 H.
Multi-solitons of a (2+1)- dimensional vector soliton system Ken-ichi Maruno Department of Mathematics, University of Texas -- Pan American Joint work.
1 Steklov Mathematical Institute RAS G. Alekseev G. Alekseev Cosmological solutions Dynamics of waves Fields of accelerated sources Stationary axisymmetric.
Gravitational and electromagnetic solitons Stationary axisymmetric solitons; soliton waves Monodromy transform approach Solutions for black holes in the.
Math 3120 Differential Equations with Boundary Value Problems Chapter 2: First-Order Differential Equations Section 2-5: Solutions By Substitution.
1 Beginning & Intermediate Algebra – Math 103 Math, Statistics & Physics.
On Matrix Painleve Systems Yoshihiro Murata Nagasaki University 20 September 2006 Isaac Newton Institute.
Aaron Barker DEFINITION OF THE DERIVATIVE.  The Definition of the Derivative can be used to find the derivative of polynomials and exponential functions.
CLASSICAL INTEGRABLE STRUCTURES IN QUANTUM INTEGRABLE MODELS joint work with V.Kazakov and A.Sorin Leiden, 14 April 2010 based on A.Zabrodin (ITEP, Moscow)
Dmitry Arkhipov and Georgy Khabakhpashev New equations for modeling nonlinear waves interaction on a free surface of fluid shallow layer Department of.
Belinski and Zakharov (1978) -- Inverse Scattering Method -- Soliton solutions on arbit. backgr. -- Riemann – Hilbert problem + linear singular integral.
Notes Over 7.6 Solving a Simple Radical Equation Solve the equation. Check your solution.
How do you check for extraneous solutions? -=. In this lesson you will learn to identify extraneous solutions in rational equations by checking solutions.
Linear Constant-Coefficient Difference Equations
1 Beginning & Intermediate Algebra – Math 103 Math, Statistics & Physics.
1 Numbers & Basic Algebra – Math 103 Math, Statistics & Physics.
Addition Math Facts = 9. Addition Math Facts = 1 5.
Algebra Core Review. Unit 1: Real Numbers Natural Numbers: Whole Numbers: Integers:
Company LOGO Laplace Transform Ch # 5 1. Company LOGO Topics 1. Get to know: Laplace Transform 2. Laplace Theory and Properties 3. Applications 2.
case study on Laplace transform
Advanced Engineering Mathematics 6th Edition, Concise Edition
Math Facts.
Warm-up Multiply the factors and write in standard form.
Finding Real Roots of Polynomial Equations
3-1 Graphing Systems of Equations
MATH 450 Enthusiastic Study/snaptutorial.com
Notes Over 9.6 An Equation with One Solution
Other Types of Equations
Linear Equations and Rational Equations
Solving Linear Systems Algebraically
paraxial approximation
Chapter IV Gauge Field Lecture 1 Books Recommended:
Algebra II Honors/Gifted
3.4 Zeros of Polynomial Functions: Real, Rational, and Complex
B.Sc. II Year Mr. Shrimangale G.W.
Introduction to bilinear method
Lie point symmetry Applications. Motivation The concept of symmetry fascinated through the centuries many artists and scientists, from the Greeks to Kepler,
Addition Math Facts (Facts to 10, 15, & 20)
Solving Equations 3x+7 –7 13 –7 =.
Solving Trigonometric Equations by Algebraic Methods
Solve Radical Equations and Inequalities
Y. Sumino (Tohoku Univ.) Evaluation of Master Integrals:
Hosted by Type your name here
11-5 Solving Rational Equations
Common Core Vs Kansas Standards
Solitons.
Presentation transcript:

From the KP hierarchy to the Painlevé equations Painlevé Equations and Monodromy Problems: Recent Developments From the KP hierarchy to the Painlevé equations Saburo KAKEI (Rikkyo University) Joint work with Tetsuya KIKUCHI (University of Tokyo) 22 September 2006

Known Facts Fact 1 Painlevé equations can be obtained as similarity reduction of soliton equations. Fact 2 Many (pahaps all) soliton equations can be obtained as reduced cases of Sato’s KP hierarchy.

Similarity reduction of soliton equations E.g. Modified KdV equation Painlevé II mKdV hierarchy Modified KP hierarchy mKdV eqn. Painlevé II: Similarity

Noumi-Yamada (1998) Lie algebra Soliton eqs. → Painlevé eqs. mKdV Panlevé II mBoussinesq Panlevé IV 3-reduced KP Panlevé V ・・・ n-reduced KP Higher-order eqs.

Aim of this research Consider the “multi-component” cases. Multi-component KP hierarchy = KP hierarchy with matrix-coefficients

Higher-order eqs. [Noumi-Yamada] From mKP hierarchy to Painlevé eqs. mKP reduction Soliton eqs. Painlevé eqs. 1-component 2-reduced mKdV P II 3-reduced mBoussinesq P IV 4-reduced 4-reduced KP P V n-reduced n-reduced KP Higher-order eqs. [Noumi-Yamada] 2-component (1,1) NLS P IV [Jimbo-Miwa] (2,1) Yajima-Oikawa P V [Kikuchi-Ikeda-K] 3-component (1,1,1) 3-wave system P VI [K-Kikuchi] …

Relation to affine Lie algebras realization mKP soliton Painlevé Principal 1-component, 2-reduced mKdV P II Homogeneous 2-component, (1,1)-reduced NLS P IV 1-component, 3-reduced mBoussinesq (2,1)-graded 2-component, (2,1)-reduced Yajima-Oikawa P V 3-component, (1,1,1)-reduced 3-wave P VI

Rational solutions of Painlevé IV Schur polynomials Rational sol’s of P IV 1-component KP mBoussinesq P IV “3-core” Okamoto polynomials [Kajiwara-Ohta], [Noumi-Yamada] 2-component KP derivative NLS P IV “rectangular” Hermite polynomials [Kajiwara-Ohta], [K-Kikuchi]

Aim of this research Consider the multi-component cases. Consider the meaning of similarity conditions at the level of the (modified) KP hierarchy.

Multi-component mKP hierarchy Shift operator Sato-Wilson operators Sato equations

1-component mKP hierarchy mKdV 2-reduction (modified KdV eq.)

Scaling symmetry of mKP hierarchy Proposition 1 Define as  where satisfies Then also solve the Sato equations.

1-component mKP mKdV P II 2-reduction (mKP mKdV) Similarity condition (mKdV P II)

2-component mKP NLS P IV (1,1)-reduction (2c-mKP NLS) Similarity condition (NLS P IV)

Parameters in similarity conditions Parameters in Painlevé equations mKdV case (P II) NLS case (P IV)

Monodromy problem Similarity condition (NLS P IV)

Aim of this research Consider the multi-component cases. Consider the meaning of similarity conditions at the level of the (modified) KP hierarchy. Consider the 3-component case to obtain the generic Painlevé VI.

Painlevé VI as similarity reduction Three-wave interaction equations  [Fokas-Yortsos], [Gromak-Tsegelnik], [Kitaev], [Duburovin-Mazzoco], [Conte-Grundland-Musette], [K-Kikuchi] Self-dual Yang-Mills equation  [Mason-Woodhouse], [Y. Murata], [Kawamuko-Nitta] Schwarzian KdV Hierarchy  [Nijhoff-Ramani-Grammaticos-Ohta], [Nijhoff-Hone-Joshi] UC hierarchy [Tstuda], [Tsuda-Masuda] D4(1)-type Drinfeld-Sokolov hierarchy [Fuji-Suzuki] Nonstandard 2 2 soliton system [M. Murata]

Painlevé VI as similarity reduction Direct approach based on three-wave system [Fokas-Yortsos (1986)] 3-wave PVI with 1-parameter [Gromak-Tsegelnik (1989)] 3-wave PVI with 1-parameter [Kitaev (1990)] 3-wave PVI with 2-parameters [Conte-Grundland-Musette (2006)] 3-wave PVI with 4-parameters (arXiv:nlin.SI/0604011)

Our approach (arXiv:nlin.SI/0508021) 3-component KP hierarchy (1,1,1)-reduction gl3-hierarhcy Similarity reduction 3×3 monodromy problem Laplace transformation 2×2 monodromy problem

3-component KP 3-wave system Compatibiliry

3-component KP 3-wave system (1,1,1)-condition: 3-wave system

3-component KP 3 3 system (1,1,1)-reduction Similarity condition cf. [Fokas-Yortsos]

3-component KP 3 3 system Similarity condition

3-component KP 3 3 system

3 3 2 2 [Harnad, Dubrovin-Mazzocco, Boalch] 3 3 2 2 [Harnad, Dubrovin-Mazzocco, Boalch] Laplace transformation with the condition :

Our approach (arXiv:nlin.SI/0508021) 3-component KP hierarchy (1,1,1)-reduction gl3-hierarhcy Similarity reduction 3×3 monodromy problem Laplace transformation 2×2 monodromy problem P VI

q-analogue (arXiv:nlin.SI/0605052) 3-component q-mKP hierarchy (1,1,1)-reduction q-gl3-hierarhcy q-Similarity reduction 3×3 connection problem q-Laplace transformation 2×2 connection problem q-P VI

References SK, T. Kikuchi, The sixth Painleve equation as similarity reduction of gl3 hierarchy, arXiv: nlin.SI/0508021 SK, T. Kikuchi, A q-analogue of gl3 hierarchy and q-Painleve VI, arXiv:nlin.SI/0605052 SK, T. Kikuchi, Affine Lie group approach to a derivative nonlinear Schrödinger equation and its similarity reduction, Int. Math. Res. Not. 78 (2004), 4181-4209 SK, T. Kikuchi, Solutions of a derivative nonlinear Schrödinger hierarchy and its similarity reduction, Glasgow Math. J. 47A (2005) 99-107 T. Kikuchi, T. Ikeda, SK, Similarity reduction of the modified Yajima-Oikawa equation, J. Phys. A36 (2003) 11465-11480