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Stochastic Description of Quantum Dissipative Dynamics Jiushu Shao Beijing Normal University 11 August 2010 Physics and Chemistry in Quantum Dissipative.

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Presentation on theme: "Stochastic Description of Quantum Dissipative Dynamics Jiushu Shao Beijing Normal University 11 August 2010 Physics and Chemistry in Quantum Dissipative."— Presentation transcript:

1 Stochastic Description of Quantum Dissipative Dynamics Jiushu Shao Beijing Normal University 11 August 2010 Physics and Chemistry in Quantum Dissipative Systems YITP, Kyoto University

2 Outline  Motives  Stochastic Formulation of Dissipative Systems  Analytical and Numerical Results  Summary

3 Molecular Chirality Why are the chiral configurations stable?

4 Quantum Control of Chirality Wang & JS, PRA 49, R637 (1994); JS & Hanggi, PRA 56, R4397 (1997); JCP 107, 9935 (1997)

5 Multidimensional Dynamics MD: large systems, no quantum effect  MD: large systems, no quantum effect Difficulties of quantum dynamics  Difficulties of quantum dynamics Schrödinger rep : memory bottleneck Schrödinger rep : memory bottleneck Path integral: Sign problem Path integral: Sign problem Curse of Dimensionality

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7 Dynamics of Open Systems Projection Operator Nakajima (1958) Zwanzig (1960) Mori (1965) Influence Functional Feynman & Vernon (1963) Caldeira & Leggett (1983) Weiss’s Book (1993, 1999) Stochastic Description Kubo & Tanimura Stockburger & Grabert (2001) Shao (2004)

8 Microscopic Description  Hamiltonian  Propagator of Whole System  Interaction Term

9 Decoupling Interaction in Real Time Evolution JS, JCP 120, 5053 (2004); Castin, Dalibard, Chomaz Hubbard-Stratonovich Transformation

10 Propagator JS, JCP 120, 5053 (2004); Chem Phys 370, 29 (2010)

11 Gaussian Fields  Statistical Properties for  Separated Hamiltonians White Noise

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13 Equation of Motion (EOM)  Initial Condition  Decoupled Equations of Motion  Change of Variables

14 EOM  Reduced Density Matrix (RDM)  Trace of the Density Matrix for the Bath

15 Girsanov Transformation  RDM  Change of Variables  EOM

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17 Primary Numerics

18 Bath-induced Random Field  Caldeira-Leggett Model  Response Function

19 Master Equation  Furutsu-Novikov Theorem  Exact “Master Equation”

20 Formal Solution of Random Density Matrix JS, Chem. Phys. 322, 187 (2006), 370, 29 (2010) correspond to correspond to

21 Formal Solution of Auxiliary Operators  Time-Local Form  Time-Nonlocal Form

22 Markovian Limit  Exact Relation  Approximation  Master Equation

23 Spontaneous Decay of Two-State Atoms  Hamiltonian  Bath-Induced Field

24 Number of Samplings : 2^24

25 Hierarchy Scheme Yan, Yang, Liu, & JS, CPL 395, 216 (2004), Tanimura, Cao, Yan  Memory Kernel  Auxiliary Quantities  EOM  Truncation

26  Bath-Induced Field  Auxiliary Quantities

27 Hierarchical Structure

28 Truncation vs Dissipation Strength Zhou, Yan & JS, EPL 72, 305 (2005), YiJing Yan

29 Truncation vs Memory Length

30 Rev. Mod. Phys. 59, 1 (1987)

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32 Mixed Random-Hierarchy Approach Zhou, Yan & JS, EPL 72, 334 (2005)

33 Special Case ( α = 0.5)

34 Decay Dynamics (α> 0.5) Zhou & JS, JCP 128, 034106 (2008)

35 Decay Rate

36 Phase Diagram

37 Summary  Establishing a stochastic formulation of quantum dissipative dynamics  Deriving master equations  Developing numerical techniques  Studying spin-boson model

38 Acknowledgements  Dr. Yun-an Yan , Dr. Yun Zhou, Dr. Yu Liu , Fan Yang, and Dr. Wenkai Zhang  Profs. X.Q. Li, U. Weiss, Y.J. Yan  National Natural Science Foundation of China  Chinese Academy of Sciences

39 Thank You

40 Dissipative Systems

41 Electron Transfer Yan, Yang, Liu, & JS, CPL 395, 216 (2004) Model: Spectral Density Function A finite number N e of exponentials will be used in numerical calculations.

42 Transient Dynamics

43 Rate Constants

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