Solution of Faddeev Integral Equations in Configuration Space Walter Gloeckle, Ruhr Universitat Bochum George Rawitscher, University of Connecticut Fb-18,

Slides:



Advertisements
Similar presentations
Stokes Phenomena and Non-perturbative Completion in the multi-cut matrix models Hirotaka Irie (NTU) A collaboration with Chuan-Tsung Chan (THU) and Chi-Hsien.
Advertisements

Ionization of the Hydrogen Molecular Ion by Ultrashort Intense Elliptically Polarized Laser Radiation Ryan DuToit Xiaoxu Guan (Mentor) Klaus Bartschat.
Introduction to Molecular Orbitals
MEASURES OF POST-PROCESSING THE HUMAN BODY RESPONSE TO TRANSIENT FIELDS Dragan Poljak Department of Electronics, University of Split R.Boskovica bb,
A novel approach to include pp Coulomb force into the 3N Faddeev calculations H. Witała, R. Skibiński, J. Golak Jagiellonian University W. Gloeckle Ruhr.
Three-nucleon force effects in proton- deuteron scattering Souichi Ishikawa (Hosei University) FB19, Aug Sep. 5, Bonn.
Photodisintegration of in three dimensional Faddeev approach The 19th International IUPAP Conference on Few-Body Problems in Physics S. Bayegan M. A. Shalchi.
Matlab Matlab is a powerful mathematical tool and this tutorial is intended to be an introduction to some of the functions that you might find useful.
Shape resonances localization and analysis by means of the Single Center Expansion e-molecule scattering theory Andrea Grandi and N.Sanna and F.A.Gianturco.
Copy and complete using a review term from the list below.
III Solution of pde’s using variational principles
Method of Hyperspherical Functions Roman.Ya.Kezerashvili New York City Technical College The City University of New York.
Pseudospectral Methods
Ch 23 pages Lecture 15 – Molecular interactions.
Simulation of radiative heat transfer in participating media with simplified spherical harmonics Ralf Rettig, University of Erlangen Ferienakademie Sarntal.
Hydrogen molecular ion in a strong magnetic field by the Lagrange-mesh method Cocoyoc, February 2007 Daniel Baye Université Libre de Bruxelles, Belgium.
Mathematical Models and Numerical Investigation for the Eigenmodes of the Modern Gyrotron Resonators Oleksiy KONONENKO RF Structure Development Meeting,
Boyce/DiPrima 9 th ed, Ch 11.5: Further Remarks on Separation of Variables: A Bessel Series Expansion Elementary Differential Equations and Boundary Value.
Y. Ikeda and T. Sato (Osaka Univ.) ストレンジ・ダイバリオンの 質量と崩壊幅の研究 KNN resonance (Recent theoretical progress) KNN resonance (Recent theoretical progress) Faddeev.
Numerical ElectroMagnetics & Semiconductor Industrial Applications Ke-Ying Su Ph.D. National Central University Department of Mathematics 11 NUFFT & Applications.
Meeting 11 Integral - 3.
MATLAB Basics. The following screen will appear when you start up Matlab. All of the commands that will be discussed should be typed at the >> prompt.
Lecture Objectives: Analyze the unsteady-state heat transfer Conduction Introduce numerical calculation methods Explicit – Implicit methods.
Goal: Solve a system of linear equations in two variables by the linear combination method.
6. Introduction to Spectral method. Finite difference method – approximate a function locally using lower order interpolating polynomials. Spectral method.
A Real-Time Numerical Integrator for the Spring 2004 Scientific Computing – Professor L. G. de Pillis A Real-Time Numerical Integrator for the One-Dimensional.
Takuma Matsumoto (Kyushu Univ.) K. Minomo, K. Ogata a, M. Yahiro, and K. Kato b (Kyushu Univ, a RCNP, b Hokkaido Univ) Description for Breakup Reactions.
Matrix Models and Matrix Integrals A.Mironov Lebedev Physical Institute and ITEP.
Three-Body Scattering Without Partial Waves Hang Liu Charlotte Elster Walter Glöckle.
1 Complex Images k’k’ k”k” k0k0 -k0-k0 branch cut   k 0 pole C1C1 C0C0 from the Sommerfeld identity, the complex exponentials must be a function.
The Double Pendulum by Franziska von Herrath & Scott Mandell.
Application of coupled-channel Complex Scaling Method to Λ(1405) 1.Introduction Recent status of theoretical study of K - pp 2.Application of ccCSM to.
Quantum Two 1. 2 Evolution of Many Particle Systems 3.
Accuracy of the Relativistic Distorted-Wave Approximation (RDW) A. D. Stauffer York University Toronto, Canada.
Physics 361 Principles of Modern Physics Lecture 11.
Application of correlated basis to a description of continuum states 19 th International IUPAP Conference on Few- Body Problems in Physics University of.
Multichannel Quantum Defect Theory -The Brief Introduction - Department of Chemistry Kim Ji-Hyun.
6.9 Dirichlet Problem for the Upper Half-Plane Consider the following problem: We solved this problem by Fourier Transform: We will solve this problem.
Do Now (3x + y) – (2x + y) 4(2x + 3y) – (8x – y)
Math 7 Combine Like Terms. Title: Combine Like Terms Objective: To combine like terms EQ: How do I combine Like Terms? In your INB, Page.
Physics “Advanced Electronic Structure”
Nicolas Michel CEA / IRFU / SPhN / ESNT April 26-29, 2011 Isospin mixing and the continuum coupling in weakly bound nuclei Nicolas Michel (University of.
Differential Equations Linear Equations with Variable Coefficients.
Klein-Gordon Equation in the Gravitational Field of a Charged Point Source D.A. Georgieva, S.V. Dimitrov, P.P. Fiziev, T.L. Boyadjiev Gravity, Astrophysics.
Physics Lecture 11 3/2/ Andrew Brandt Monday March 2, 2009 Dr. Andrew Brandt 1.Quantum Mechanics 2.Schrodinger’s Equation 3.Wave Function.
Resonance states of relativistic two-particle systems Kapshai V.N., Grishechkin Yu.A. F. Scorina Gomel State University.
Faddeev Calculation for Neutron-Rich Nuclei Eizo Uzu (Tokyo Univ. of Science) Collaborators Masahiro Yamaguchi (RCNP) Hiroyuki Kamada (Kyusyu Inst. Tech.)
Central potential problem and angular momentum What is a central potential? Separating the Angular and Radial wave equations Asymptotics of the radial.
OSC 2nd Annual Graduate Student HPC Workshop 1 Three-Body Bound State Calculations with Two and Three-Body Forces Hang Liu Charlotte Elster Department.
Adiabatic hyperspherical study of triatomic helium systems
Possible molecular bound state of two charmed baryons - hadronic molecular state of two Λ c s - Wakafumi Meguro, Yan-Rui Liu, Makoto Oka (Tokyo Institute.
Notes 6.5, Date__________ (Substitution). To solve using Substitution: 1.Solve one equation for one variable (choose the variable with a coefficient of.
APS April Meeting 2002 The Dynamics of Three Body Forces in Three Nucleon Bound State Hang Liu Charlotte Elster Walter Glöckle.
Numerical Solutions of Partial Differential Equations CHAPTER 16.
Matrices and Linear Systems Roughly speaking, matrix is a rectangle array We shall discuss existence and uniqueness of solution for a system of linear.
E. Todesco, Milano Bicocca January-February 2016 Appendix A: A digression on mathematical methods in beam optics Ezio Todesco European Organization for.
Lecture Objectives: - Numerics. Finite Volume Method - Conservation of  for the finite volume w e w e l h n s P E W xx xx xx - Finite volume.
Tunneling Ionization of Hydrogen atom in an Electric Field Hillary Ssemanda 森下研.
Theory of Scattering Lecture 3. Free Particle: Energy, In Cartesian and spherical Coordinates. Wave function: (plane waves in Cartesian system) (spherical.
Three-body calculation of the 1s level shift in kaonic deuterium
Differential Equations
Solving Equations by Factoring and Problem Solving
المحاضرة السادسة حل معادلة شرود نجر في بعد واحد (1) الجهد اللانهائي
§3.3.1 Separation of Cartesian variables: Orthogonal functions
Solving Linear Systems Algebraically
ME/AE 339 Computational Fluid Dynamics K. M. Isaac Topic2_PDE
Do all the reading assignments.
Solving Systems of Equations by Elimination Part 2
Spherical Bessel Functions
R. Lazauskas Application of the complex-scaling
Presentation transcript:

Solution of Faddeev Integral Equations in Configuration Space Walter Gloeckle, Ruhr Universitat Bochum George Rawitscher, University of Connecticut Fb-18, Santos, Brazil, August 24, 2006 Work in Progress physics/ ;

AIM: Solve three-body problems for Atomic Physics Method: 1.Use Faddeev Equations in Configuration space 2.Use only integral equations for the product potential x Wave function, called T 3.Numerical discretization via the Spectral expansion in terms of Chebyshev Polynomials

12 3 x1x1 y1y1

Two-Body Three-Body T = Product of wave function times potential t or  t - matrix

Two-b T-matrix imbedded in three-b space Two-body Three-body free Green’s function Two-body free Green’s function

Differential Fad’v Eq. for the wave fctn. Integral Fad’v Eq for the wave fctn. Integral Fad’v Eq for the T - fctn.

Coupled Faddeev Eqs. With 3b-Pot’l A big mess, that requires the two-body t-matrices t i I = 1, 2, 3

Two-b tau-matrix, one dimension Two variables

Spectral Integral Equation Method 12 i j Partitions Result: Obtain a Rank 2 separable expression

0 < r < 3000 a.u. He-He binding energy via the S-IEM Rawitscher and Koltracht, Eur. J. Phys. 27, 1179 (2006)

Computing time for MATLAB (sec) with S-IEM 2.8 GHz Intel computer, 200 Partitions, 17 points per partition S-IEM

Next Steps: toy model 2. Ignore the three-body interaction, and solve for identical particles 1. Go to the configuration representation 3. Make a partial wave exp.; set all L= 0

Ansatz: Basis Functions

He-He bound state

Chebyshev expansion of v * Psi for He-He bound state 3.5 < r < 40

Equations for the expansion coefficients Final Matrix eqs.

Complexity Estimates # of coordinate points # of basis functions # of angles # of partitions and q values Additional computational factor

Ingredients for the Toy Model matrix eq. Solution of the matrix eq. 1-2 Hours Fortran on a 2 GHz PC

Summary and Conclusions Integral Faddeev Eqs. in Config. Space for T(x,y) = V x Psi, combined with the spectral method for solving integral equations; Greens function incorporate asymptotic boundary conditions; Toy model should take about one hour The expected accuracy is more than 6 sign. figs.