EQUATION LANGEVIN. Physics, Chemistry and Electrical Engineering. World Scientific. With Applications to Stochastic Problems in. William T.

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SHANGHAI HONG WorlrfScientific Series krtonttimfjorary Chemical Physics-Vol. 27 THE LANGEVIN EQUATION With Applications to Stochastic Problems in Physics, Chemistry and Electrical Engineering Third Edition William T. Coffey Trinity College, Ireland Yuri P. Kalmykov Universite de Perpignan Via Domitia, France World Scientific NEW JERSEY LONDON SINGAPORE BEIJING KONG TAIPEI CHENNAI

CONTENTS Preface to the Third Edition Contents vii xv Chapter 1 Historical Background and Introductory Concepts 1 1.1. Brownian motion 1 1.2. Einstein's explanation of Brownian movement 5 1.3. The Langevin equation 10 1.3.1. Calculation of Avogadro's number 14 1.4. Einstein's Method 16 1.5. Essential concepts in Statistical Mechanics 21 1.5.1. Ensemble of systems 23 1.5.2. Phase space 23 1.5.3. Representative point 24 1.5.4. Ergodic hypothesis 24 1.5.5. Calculation of averages 25 1.5.6. Liouville equation 27 1.5.7. Reduction of the Liouville equation 28 1.5.8. Langevin equation for a system with one degree of freedom 29 1.5.9. Intuitive derivation of the Klein-Kramers equation 30 1.5.10. Conditions under which a Maxwellian distribution in the may be deemed to be attained 32 1.5.11. Very-high-damping (VHD) regime 33 1.5.12. Very-low-damping (VLD) regime 38 1.6. Probability theory 42 1.6.1. Random variables and probability distributions 43 1.6.2. The Gaussian distribution -.45 1.6.3. Moment-generating functions 48 1.6.4. Central limit theorem 52 1.6.5. Random processes 53 1.6.6. Wiener-Khinchin theorem 55 1.7. Application to the Langevin equation 56 1.8. Wiener process 58 1.8.1. Variance of the Wiener process 59 1.8.2. Wiener integrals 61 1.9. The Fokker-Planck equation 63 1.10. Drift and diffusion coefficients 69 xv

xvi The Langevin Equation 1.11. Solution of the one-dimensional Fokker-Planck equation 72 1.12. The Smoluchowski equation 75 1.13. Escape of particles over potential barriers: Kramers' theory 77 1.13.1. Escape rate in the IHD limit 83 1.13.2. Kramers' calculation of the escape rate in the VLD limit 87 1.13.3. Range of validity of the IHD and VLD formulas 90 1.13.4. Extension of Kramers' theory to many dimensions in the IHD limit 92 1.13.5. Langer's treatment of the IHD limit 94 1.13.6. Kramers' formula as a special case of Langer's formula 99 1.13.7. Kramers'turnover problem 101 1.14. Applications of the theory of Brownian movement in a potential 112 1.15. Rotational Brownian motion: application to dielectric relaxation 114 1.15.1. Breakdown of the Debye theory at high frequencies 118 1.16. Superparamagnetism: magnetic after-effect 121 1.17. Brown's treatment of Neel relaxation 128 1.18. Asymptotic expressions for the Neel relaxation time 132 1.18.1. Magnetization reversal time in a uniaxial superparamagnet: application of Kramers' method 132 1.18.2. Escape rate formulas for superparamagnets 136 1.19. Ferrofluids 141 1.20. Depletion effect in a biased bistable potential./. 143 1.21. Stochastic resonance 149 1.22. Anomalous diffusion 151 1.22.1. Empirical formulas for the complex dielectric permittivity 156 1.22.2. Theoretical justification for anomalous relaxation behavior 157 1.22.3. Anomalous dielectric relaxation of an assembly of dipolar molecules 160 References 163 Chapter 2 Langevin Equations and Methods of Solution 171 2.1. Criticisms ofthe Langevin equation 171 2.2. Doob's interpretation of the Langevin equation 172 2.3. Nonlinear Langevin equation with a multiplicative noise term: Ito and Stratonovich rules 174 2.4. Derivation of differential-recurrence relations from the one-dimensional Langevin equation 178 2.5. Nonlinear Langevin equation in several dimensions 180 2.6. Average of me multiplicative noise term in the Langevin equation 183 2.6.1. Multiplicative noise term for rotation in space 185 2.6.2. Multiplicative noise terms in the non-inertial limit 186 2.6.3. Explicit average of the noise-induced terms for a planar rotator 188

Contents xvii 2.7. Methods of solution of differential-recurrence relations arising from the nonlinear Langevin equation 190 2.7.1. Matrix method 191 2.7.2. Initial conditions 193 2.7.3. Matrix continued-fraction solution of recurrence equations 195 2.8. Linear response theory 201 2.9. Integral relaxation time 206 2.10. Linear response theory for systems with dynamics governed by singlevariable Fokker-Planck equations 208 2.11. Smallest non-vanishing eigenvalue: continued-fraction approach 212 2.11.1 Evaluation of A\ from a scalar three-term recurrence relation 213 2.11.2 Evaluation of Ai from a matrix three-term recurrence relation 216 2.12. Effective relaxation time 218 2.13. Evaluation of the dynamic susceptibility using zmx, ref, and Xx 220 2.14. Nonlinear transient response of a Brownian particle 222 References 225 Chapter 3 Brownian Motion of a Free Particle and a Harmonic Oscillator 229 3.1. Introduction 229 3.2. Ornstein-Uhlenbeck theory ofbrownian motion 230 3.3. Stationary solution of the Langevin equation: the Wiener-Khinchin theorem 231 3.4. Application to phase diffusion in MRI 235 3.5. Brownian motion of a harmonic oscillator 241 3.6. Rotational Brownian motion of a fixed-axis rotator 243 3.7. Torsional oscillator model: example of the use of the Wiener integral 246 References 250 Chapter 4 Rotational Brownian Motion About a Fixed Axis in A'-Fold Cosine Potentials 253 4.1. Introduction 253 4.2. Langevin equation for rotation about a fixed axis 254 4.3. Longitudinal and transverse effective relaxation times 257 4.4. Polarizabilities and relaxation times of a fixed-axis rotator with two equivalent sites 261 4.4.1. Matrix solution for the longitudinal response 263 4.4.2. Continued-fraction solution for the longitudinal response 265 4.4.3. Comparison of the longitudinal relaxation time with the Kramers theory 271 4.4.4. Continued-fraction solution for the transverse response 272 4.5. Effect ofa d.c. bias field on the orientational relaxation of a fixed-axis rotator with two equivalent sites 277 4.5.1. Longitudinal response 277

xviii The Langevin Equation 4.5.2. Transverse response 280 4.5.3. Relaxation times 281 References 283 Chapter 5 Brownian Motion in a Tilted Periodic Potential: Application to the Josephson Tunnelling Junction 285 5.1. Introduction 285 5.2. Langevin equations 286 5.3. Josephson junction: dynamic model 287 5.4. Reduction of the averaged Langevin equation for the junction to a set of differential-recurrence relations 290 5.5. Current-voltage characteristics 293 5.6. Linear response to an applied alternating current 298 5.7. Effective eigenvalues for the Josephson junction 300 5.8. Linear impedance 303 5.9. Spectrum of the Josephson radiation 307 5.10. Nonlinear effects in d.c. and a.c. current-voltage characteristics 310 5.11. Concluding remarks 317 References 318 Chapter 6 Translational Brownian Motion in a Double-Well Potential 321 6.1. Introduction 321 6.2. Characteristic times of the position correlation function 323 6.3. Converging continued fractions for the correlation functions 332 6.4. Two-mode approximation 336 6.5. Stochastic resonance 338 6.6. Concluding remarks 340 References 340 Chapter 7 Non-inertial Rotational Diffusion in Axially Symmetric External Potentials: Applications to Orientational Relaxation of Molecules in Fluids and Liquid Crystals 343 7.1. Introduction 343 7.2. Rotational diffusion in a potential: Langevin equation approach 344 7.2.1. Averaging the non-inertial Euler-Langevin equation 346 7.2.2. Differential-recurrence equations for spherical harmonics 348 7.2.3. Examples of differential-recurrence equations 350 7.3. Brownian rotation in a uniaxial potential 352 7.3.1. Longitudinal relaxation 355 7.3.2. Susceptibility and relaxation times: continued-fraction solution 358 7.3.3. Integral form and asymptotic expansions of the exact solution 363 7.3.4. Transverse response: continued-fraction solution 365 7.3.5. Complex susceptibilities 368

Contents xix 7.4. Brownian rotation in a uniform d.c. external field 372 7.4.1. Longitudinal response: continued-fraction solution 374 7.4.2. Transverse response: continued-fraction solution 377 7.4.3. Comparison with experimental data 380 7.5. Nonlinear transient responses in dielectric and Kerr-effect relaxation 382 7.5.1. Nonlinear transient dielectric and Kerr-effect relaxation times 384 7.5.2. Nonlinear step-on transient response: matrix continued-fraction solution 387 7.6. Nonlinear dielectric relaxation of polar molecules in a strong a.c. electric field: steady-state response 392 7.7. Concluding remarks 397 References 398 Chapter 8 Anisotropic Non-inertial Rotational Diffusion in an External Potential: Application to Linear and Nonlinear Dielectric Relaxation and the Dynamic Kerr Effect 403 8.1. Introduction 403 8.2. Anisotropic non-inertial rotational diffusion of an asymmetric top in an external potential 404 8.2.1. Euler-Langevin equation in the non-inertial limit 404 8.2.2. Differential-recurrence equation for Wigner's D functions 408 8.3. Application to dielectric relaxation 413 8.3.1. Linear dielectric response of an assembly of asymmetric tops 413 8.3.2. Nonlinear response in superimposed a.c. and strong d.c. bias fields: perturbation solution 415 8.3.3. Rotational Brownian motion and dielectric relaxation in nematic liquid crystals 418 8.4. Kerr-effect relaxation 429 8.4.1. Basic relations 431 8.4.2. Dynamic Kerr effect: matrix formulation 432 8.4.3. Nonlinear dielectric and Kerr-effect transients in strong fields 447 8.5. Concluding remarks 453 References 454 Chapter 9 Brownian Motion of Classical Spins: Application to Magnetization Relaxation in Superparamagnets 459 9.1. Introduction 459 9.2. Brown's model: Langevin equation approach 462 9.2.1. Derivation of the differential-recurrence equation for the statistical moments from the stochastic Gilbert equation 464 9.2.2. Fokker-Planck equation approach 467 9.2.3. Differential-recurrence equations for a uniaxial superparamagnet in an external magnetic field 469

XX The Langevin Equation 9.2.4. Comparison of the Gilbert, Landau-Lifshitz, and Kubo kinetic models of the Brownian rotation of classical spins 470 9.2.5. Calculation of the observables 473 9.3. Magnetization relaxation in uniaxial superparamagnets 477 9.3.1. Longitudinal relaxation 479 9.3.2. Characteristic times and magnetic susceptibility 483 9.3.3. Magnetic stochastic resonance 488 9.3.4. Dynamic magnetic hysteresis 493 9.3.5. Transverse response: ferromagnetic resonance 503 9.4. Reversal time of the magnetization in superparamagnets with nonaxially symmetric potentials: escape-rate theory approach 509 9.4.1. Basic equations for the escape rate 512 9.4.2. Discrete orientation model 515 9.4.3. Reversal time for cubic anisotropy 520 9.4.4. Uniaxial superparamagnet in a uniform d.c. magnetic field 523 9.4.5. Biaxial superparamagnet in a uniform d.c. magnetic field applied along the easy axis 530 9.4.6. Mixed anisotropy: breakdown of the paraboloid approximation 532 9.4.7. Reversal time ofa superantiferromagnetic nanoparticle 542 9.4.8. Switching-field curves and surfaces 546 9.5. Magnetization relaxation in superparamagnets with non-axially symmetric anisotropy: matrix continued-fraction approach 553 9.5.1. Uniaxial superparamagnet in an oblique field 553 9.5.2. Cubic anisotropy 562 9.6. Nonlinear a.c. stationary response of superparamagnets 574 9.7. Concluding remarks 581 References» 585 Chapter 10 Inertial Effects in Rotational and Translational Brownian Motion for a Single Degree offreedom 595 10.1. Introduction 595 10.2. Inertial effects in nonlinear dielectric response 601 10.2.1. Linear response for non-inertial rotation about a fixed axis 603 10.2.2. Differential-recurrence equations for nonlinear transients 605 10.2.3. Matrix continued-fraction solution 608 10.2.4. Analytic equations for the integral relaxation time 610 10.2.5. Inertial effects 612 10.3. Brownian motion of a fixed-axis rotator in a double-well potential 616 10.3.1. Matrix continued-fraction solution 617 10.3.2. Turnover formula for the escape rate 619 10.3.3. Analytic formulas for the longitudinal correlation time 625

Contents xxi 10.4. Brownian motion of a fixed-axis rotator in an asymmetric double-well potential 629 10.4.1. Basic equations...^ 630 10.4.2. Matrix continued-fraction solution 633 10.4.3. Turnover formula for and VHD and VLD asymptotes for rb. Complex susceptibility 634 10.5. Brownian motion in a tilted periodic potential 642 10.5.1. Matrix continued-fraction solution 644 10.5.2. Turnover equation for the decay rate 648 10.6. Translational Brownian motion in a double-well potential j 652 10.6.1. Matrix continued-fraction solution 654 10.6.2. Longest and integral relaxation times. Dynamic susceptibility 657 10.7. Concluding remarks 663 References 664 Chapter 11 Inertial Effects in Rotational Diffusion in Space: Application to Orientational Relaxation in Molecular Liquids and Ferrofluids 669 11.1. Introduction 669 11.2. Inertial rotational Brownian motion of a thin rod in space 671 11.2.1. Recurrence equations for the correlation functions 671 11.2.2. First-rank correlation function 676 11.2.3. Second-rank correlation function 678 11.2.4. Orientational correlation function of an arbitrary rank / 679 11.3. Rotational Brownian motion of a symmetrical top 682 11.3.1. Recurrence equations for the correlation functions 682 11.3.2. First-and second-rank correlation functions 684 11.4. Inertial rotational Brownian motion of a rigid dipolar rotator in a uniaxial biased potential 691 11.4.1. Basic relations 691 11.4.2. Asymptotic formulas for the longest relaxation time 698 11.5. Itinerant oscillator model ofrotational motion in liquids 703 11.5.1. Generalization of the Onsager model: relation to the cage model 704 11.5.2. Dipole correlation function 710 11.5.3. Matrix continued-fraction solution for the complex susceptibility... 712 11.5.4. Comparison with experimental data 715 11.6. Application of the cage model to ferrofluids 718 Appendix A: Statistical averages of the Hermite polynomials of the components of the angular velocity for linear molecules 729 Appendix B: Averages of the components of the angular velocities 730 Appendix C: Sack's continued-fraction solution for the sphere 733 References 734

xxii The Langevin Equation Chapter 12 Anomalous Diffusion and Relaxation 739 12.1. Discrete-and continuous-time random walks 739 12.2. Fractional diffusion equation for the continuous-time random walk model 745 12.3. Solution of fractional diffusion equations 754 12.3.1. Anomalous diffusion of a fixed-axis rotator in a potential 759 12.3.2. Fractional diffusion ofa particle in a double-well potential 762 12.4. Characteristic times of anomalous diffusion 766 12.4.1. Mean first-passage time for normal diffusion 766 12.4.2. First-passage-time distribution for anomalous diffusion 770 12.4.3. Spectral definition of the characteristic times 774 12.5. Inertial effects in anomalous relaxation 777 12.5.1. Slow transport process governedby trapping 777 12.5.2. Calculation of the complex susceptibility 779 12.5.3. Comment on the use of the telegraph equation 784 12.6. Barkai and Silbey's fractional kinetic equation 786 12.6.1. Complex susceptibility 789 12.6.2. Fractional kinetic equation for the needle model 792 12.7. Anomalous diffusion in a periodic potential 797 12.8. Fractional Langevin equation 803 12.8.1. Application to phase diffusion in MRI 806 12.9. Concluding remarks 811 Appendix: Fractal dimension, anomalous exponents, and random walks 814 References 816 Index 821