Resonance states of a Liouvillian and Hofstadter’s butterfly type of singular spectrum of a collision operator for a protein chain August 10, 2010 Tomio.

Slides:



Advertisements
Similar presentations
Anderson localization: from single particle to many body problems.
Advertisements

POLLICOTT-RUELLE RESONANCES, FRACTALS, AND NONEQUILIBRIUM MODES OF RELAXATION Pierre GASPARD Brussels, Belgium J. R. Dorfman, College Park G. Nicolis,
I.L. Aleiner ( Columbia U, NYC, USA ) B.L. Altshuler ( Columbia U, NYC, USA ) K.B. Efetov ( Ruhr-Universitaet,Bochum, Germany) Localization and Critical.
Hamiltonian Chaos and the standard map Poincare section and twist maps. Area preserving mappings. Standard map as time sections of kicked oscillator (link.
Probability evolution for complex multi-linear non-local interactions Irene M. Gamba Department of Mathematics and ICES The University of Texas at Austin.
Particle acceleration in a turbulent electric field produced by 3D reconnection Marco Onofri University of Thessaloniki.
Many-body dynamics of association in quantum gases E. Pazy, I. Tikhonenkov, Y. B. Band, M. Fleischhauer, and A. Vardi.
Atomic Vibrations in Solids: phonons
Random-Matrix Approach to RPA Equations X. Barillier-Pertuisel, IPN, Orsay O. Bohigas, LPTMS, Orsay H. A. Weidenmüller, MPI für Kernphysik, Heidelberg.
Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does.
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Overview.
Physics “Advanced Electronic Structure” Lecture 3. Improvements of DFT Contents: 1. LDA+U. 2. LDA+DMFT. 3. Supplements: Self-interaction corrections,
Conical Intersections Spiridoula Matsika. The study of chemical systems is based on the separation of nuclear and electronic motion The potential energy.
No friction. No air resistance. Perfect Spring Two normal modes. Coupled Pendulums Weak spring Time Dependent Two State Problem Copyright – Michael D.
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Gas Dynamics.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Femtochemistry: A theoretical overview Mario Barbatti III – Adiabatic approximation and non-adiabatic corrections This lecture.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Chiral freedom and the scale of weak interactions.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Phase-space instability for particle systems in equilibrium and stationary nonequilibrium states Harald A. Posch Institute for Experimental Physics, University.
Many-body dynamics of association in quantum gases E. Pazy, I. Tikhonenkov, Y. B. Band, M. Fleischhauer, and A. Vardi.
Crystal Lattice Vibrations: Phonons
Molecular Modeling Fundamentals: Modus in Silico C372 Introduction to Cheminformatics II Kelsey Forsythe.
6. Second Quantization and Quantum Field Theory
System and definitions In harmonic trap (ideal): er.
Spin and Charge Pumping in an Interacting Quantum Wire R. C., N. Andrei (Rutgers University, NJ), Q. Niu (The University of Texas, Texas) Quantum Pumping.
Instanton representation of Plebanski gravity Eyo Eyo Ita III Physics Department, US Naval Academy Spanish Relativity Meeting September 10, 2010.
Program on « NONEQUILIBRIUM STEADY STATES » Institut Henri Poincaré 10 September - 12 October 2007 Pierre GASPARD Center for Nonlinear Phenomena and Complex.
Berry Phase Effects on Bloch Electrons in Electromagnetic Fields
Origin, Evolution, and Signatures of Cosmological Magnetic Fields, Nordita, June 2015 Evolution of magnetic fields in large scale anisotropic MHD flows.
Chang-Kui Duan, Institute of Modern Physics, CUPT 1 Harmonic oscillator and coherent states Reading materials: 1.Chapter 7 of Shankar’s PQM.
HYDRODYNAMIC MODES AND NONEQUILIBRIUM STEADY STATES Pierre GASPARD Brussels, Belgium J. R. Dorfman, College Park S. Tasaki, Tokyo T. Gilbert, Brussels.
Electronic Conduction of Mesoscopic Systems and Resonant States Naomichi Hatano Institute of Industrial Science, Unviersity of Tokyo Collaborators: Akinori.
6. Free Electron Fermi Gas Energy Levels in One Dimension Effect of Temperature on the Fermi-Dirac Distribution Free Electron Gas in Three Dimensions Heat.
Quantum Two 1. 2 Time Independent Approximation Methods 3.
LUTTINGER LIQUID Speaker Iryna Kulagina T. Giamarchi “Quantum Physics in One Dimension” (Oxford, 2003) J. Voit “One-Dimensional Fermi Liquids” arXiv:cond-mat/
XII Nuclear Physics Workshop Maria and Pierre Curie: Nuclear Structure Physics and Low-Energy Reactions, Sept , Kazimierz Dolny, Poland Self-Consistent.
Symmetries in Nuclei, Tokyo, 2008 Symmetries in Nuclei Symmetry and its mathematical description The role of symmetry in physics Symmetries of the nuclear.
1 Heat Conduction in One- Dimensional Systems: molecular dynamics and mode-coupling theory Jian-Sheng Wang National University of Singapore.
Yoon kichul Department of Mechanical Engineering Seoul National University Multi-scale Heat Conduction.
Anatoli Polkovnikov Krishnendu Sengupta Subir Sachdev Steve Girvin Dynamics of Mott insulators in strong potential gradients Transparencies online at
1 Three views on Landau damping A. Burov AD Talk, July 27, 2010.
Lecture IV Bose-Einstein condensate Superfluidity New trends.
Quantum dynamics of two Brownian particles
Shear Viscosity and Viscous Entropy Production in Hot QGP at Finite Density 报告人: 刘 绘 华中师范大学 粒子所.
Modern Physics (II) Chapter 9: Atomic Structure
AB INITIO DERIVATION OF ENTROPY PRODUCTION Pierre GASPARD Brussels, Belgium J. R. Dorfman, College Park S. Tasaki, Tokyo T. Gilbert, Brussels MIXING &
One and two component weakly nonlocal fluids Peter Ván BUTE, Department of Chemical Physics –Nonequilibrium thermodynamics - weakly nonlocal theories.
Mott phases, phase transitions, and the role of zero-energy states in graphene Igor Herbut (Simon Fraser University) Collaborators: Bitan Roy (SFU) Vladimir.
The quantum kicked rotator First approach to “Quantum Chaos”: take a system that is classically chaotic and quantize it.
Q UANTUM CHAOS IN THE COLLECTIVE DYNAMICS OF NUCLEI Pavel Cejnar, Pavel Stránský, Michal Macek DPG Frühjahrstagung, Bochum 2009, Germany Institute.
5. Quantum Theory 5.0. Wave Mechanics
Review of lecture 5 and 6 Quantum phase space distributions: Wigner distribution and Hussimi distribution. Eigenvalue statistics: Poisson and Wigner level.
Hisao Hayakawa (YITP, Kyoto University) Physics and chemistry in quantum dissipative systems, YITP, Kyoto University(2010/08/09) Fluctuation theorem and.
International Scientific Spring 2016
Lecture from Quantum Mechanics. Marek Zrałek Field Theory and Particle Physics Department. Silesian University Lecture 5.
HIRG 重离子反应组 Heavy Ion Reaction Group GDR as a Probe of Alpha Cluster in Light Nuclei Wan-Bing He ( 何万兵 ) SINAP-CUSTIPEN Collaborators : Yu-Gang.
Kadanoff-Baym Approach to Thermalization of Quantum Fields Akihiro Nishiyama University of Tokyo Institute of Physics.
Time Dependent Two State Problem
Stationary Perturbation Theory And Its Applications
Resonant Conduction through Mesoscopic Systems
Time-Dependent Perturbation Theory
Quantum Two Body Problem, Hydrogen Atom
Application of BCS-like Ideas to Superfluid 3-He
LECTURE 15.
QM2 Concept Test 11.1 In a 3D Hilbert space,
Hiroyuki Nojiri, Department of Physics, Okayama University
Institute for Theoretical Physics,
Presentation transcript:

Resonance states of a Liouvillian and Hofstadter’s butterfly type of singular spectrum of a collision operator for a protein chain August 10, 2010 Tomio Yamakoshi Petrosky Center for Complex Quantum Systems, University of Texas at Austin Naomichi Hatano (University of Tokyo) Kazuk Kanki (Osaka Prefecture University) Satoshi Tanaka (Osaka Prefecture University) Alien BaltanAsteroid belt

Eigenvalue Problem of Liouville-von Neumann Operators (Classical and Quantum) Still in poorly understood situation especially for unstable systems: Resonance states for the Louvillian Eigenvalue problem of the collision operators in Kinetic equations (complex eigenvalues and irreversibility) Other interesting properties (reversible dynamics): continuous spectrum, discrete spectrum, band structure, level repulsion, …

Myoglobyn Primary Structure: One-dimensional Molecular Chain 1) Resonance States of Quantum Liouvillian for Protein Chain  -helix 2) Level Repulsion and threefold degeneracy of eigenstates of the Liouvillian in the Kirkwood gaps in the asteroid belt Instability due to the resonance

・ Band spectrum in the relaxation modes for momentum disturibution Characteristic behavior of 1D system: ・ No classical limit just like the 1D classical gas ・ Rational-irrationality dependence of the spectrum in a physical parameter (Fractal structure) ⇒ Similarity to Hofstadter’s butterfly of a Hamiltonian spectrum for a 2D tight-binding model in a magnetic field I. Resonance States of Quantum Liouvillian for Protein Chain reversible process R irreversible process

Intrinsic degeneracy Liouville equation

Dispersion equation and Resonance states of Liouvillian Dispersion equation Operator equation The collision operator Kinetic equation Complex eigenvalues: Transport coefficient in irreversible process

Exciton Dimensionless Hamiltonian ratio of band width

Reduced density matrix Kinetic equation for the momentum distribution (weak coupling case) Planck distribution for the phonon resonance The collision operator in P 0 subspace: Momentum distribution function

Eigenvalue problem of the collision operator H-theorem rational irrational

qq 2m =10 m = 6 : resonance condition

Alien Baltan t > 0 t < 0 Rich structure of the entropy production

type-I type-II

type-I type-II

t -1/2 power law decayBand structure of the spectrum Spectra of the collision operator ! type-I

type-II Spectra of the collision operator

II. Level Repulsion and threefold degeneracy of eigenstates of the Liouvillian in the Kirkwood gaps in Asteroid belt Band spectrum of the Liouvillian in the restrict problem of three bodys Keplar’s third law

The sidereal coordinate The synodic coordinate Hamiltonian of the restricted three-body problem

Delaunay’s variables:

Dispersion relation for m-n mode: Threefold degeneracy

! Level repulsion The degenerate perturbation theory for resonances Mode coupling (Selection rule) Saturn’s ring?

Evidence of the threefold degeneracy

Summary (Instability due to the resonance) ・ Rich fractal structure of the resonance spectrum of the Liouvillian in a protein chain, Rational-irrationality dependence of the spectrum, Band structure ・ Rich structure of the entropy production, "Complex Spectrum Representation of the Liouvillan and Kinetic Theory in Nonequilibrium Physics," T. Petrosky, Prog. Theor. Phys. 123, 395 (2010) "Hofstadter’s butterfly type of singular spectrum of a collision operator for a model of molecular chains," T. Petrosky, N. Hatano, K. Kanki, and S. Tanaka, Prog. Theor. Phys. Supplement, No. 184, 457 (2010). ・ Quantum analogy of the spectrum of the Liouvillian in classical system, ・ Analysis of classical systems in terms of “states” in stead of “trajectories,” ・ The degenerate perturbation theory for resonance effect, level repulsion, band structure, … (classical quantization?)

2D tight-binding model + Magnetic field ( reversible process ) Dispersion relation: (dimensionless) rational or irrational Hofstadter’s butterfly Eigenvalue Problem for Hamiltonian

Hofstadter’s butterfly

Band spectrum for fixed value of R

Davydov’s interaction (k B T)/(2J) = 0.1 (k B T)/(2J) = 1 Band width of the exciton Type I Type II

Resonance states of a Liouvillian and Hofstadter’s butterfly type of singular spectrum of a collision operator for a protein chain SPQS2010, August 2, 2010 Tomio Yamakoshi Petrosky Center for Complex Quantum Systems, University of Texas at Austin Naomichi Hatano (University of Tokyo) Kazuk Kanki (Osaka Prefecture University) Satoshi Tanaka (Osaka Prefecture University) Alien BaltanAsteroid belt