A guide to the theoretical and computational toolkits for the modern study of molecular kinetics in condensed phases
Molecular Kinetics in Condensed Phases: Theory, Simulation and Analysis puts the focus on the theory, algorithms, simulations methods and analysis of molecular kinetics in condensed phases. The authors noted experts on the topic offer a detailed and thorough description of modern theories and simulation methods to model molecular events. They highlight the rigorous stochastic modelling of molecular processes and the use of mathematical models to reproduce experimental observations, such as rate coefficients, mean first passage times and transition path times.
The books exploration of simulations examines atomically detailed modelling of molecules in action and the connections of these simulations to theory and experiment. The authors also explore the applications that range from simple intuitive examples of one- and two-dimensional systems to complex solvated macromolecules. This important book:
Offers an introduction to the topic that combines theory, simulation and analysisPresents a guide written by authors that are well-known and highly regarded leaders in their fieldsContains detailed examples and explanation of how to conduct computer simulations of kinetics. A detailed study of a two-dimensional system and of a solvated peptide are discussed.Discusses modern developments in the field and explains their connection to the more traditional concepts in chemical dynamics
Written for students and academic researchers in the fields of chemical kinetics, chemistry, computational statistical mechanics, biophysics and computational biology,Molecular Kinetics in Condensed Phasesis the authoritative guide to the theoretical and computational toolkits for the study of molecular kinetics in condensed phases.
Acknowledgments xiii
Introduction: Historical Background and Recent Developments that Motivate this Book xv
1 The Langevin Equation and Stochastic Processes1
1.1 General Framework 1
1.2 The Ornstein-Uhlenbeck (OU) Process 5
1.3 The Overdamped Limit 8
1.4 The Overdamped Harmonic Oscillator: An OrnsteinUhlenbeck process 11
1.5 Differential Form and Discretization 12
1.5.1 Euler-Maruyama Discretization (EMD) and Itô Processes 15
1.5.2 Stratonovich Discretization (SD) 17
1.6 Relation Between Itô and Stratonovich Integrals 19
1.7 Space Varying Diffusion Constant 21
1.8 Itô vs Stratonovich 23
1.9 Detailed Balance 23
1.10 Memory Kernel 25
1.11 The Many Particle Case 26
References 26
2 The FokkerPlanck Equation29
2.1 The ChapmanKolmogorov Equation 29
2.2 The Overdamped Case 30
2.2.1 Derivation of the Smoluchowski (FokkerPlanck) Equation using the ChapmanKolmogorov Equation 30
2.2.2 Alternative Derivation of the Smoluchowski (FokkerPlanck) Equation 33
2.2.3 The Adjoint (or Reverse or Backward) FokkerPlanck Equation 34
2.3 The Underdamped Case 34
2.4 The Free Case 35
2.4.1 Overdamped Case 35
2.4.2 Underdamped Case 36
2.5 Averages and Observables 37
References 39
3 The Schrödinger Representation41
3.1 The Schrödinger Equation 41
3.2 Spectral Representation 43
3.3 Ground State and Convergence to the Boltzmann Distribution 44
References 47
4 Discrete Systems: The Master Equation and Kinetic Monte Carlo49
4.1 The Master Equation 49
4.1.1 Discrete-Time Markov Chains 49
4.1.2 Continuous-Time Markov Chains, Markov Processes 51
4.2 Detailed Balance 53
4.2.1 Final State Only 54
4.2.2 Initial State Only 54
4.2.3 Initial and Final State 55
4.2.4 Metropolis Scheme 55
4.2.5 Symmetrization 55
4.3 Kinetic Monte Carlo (KMC) 58
References 61
5 Path Integrals63
5.1 The Itô Path Integral 63
5.2 The Stratonovich Path Integral 66
References 67
6 Barrier Crossing69
6.1 First Passage Time and Transition Rate 69
6.1.1 Average Mean First Passage Time 71
6.1.2 Distribution of First Passage Time 73
6.1.3 The Free Particle Case 74
6.1.4 Conservative Force 75
6.2 Kramers Transition Time: Average and Distribution 77
6.2.1 Kramers Derivation 78
6.2.2 Mean First Passage Time Derivation 80
6.3 Transition Path Time: Average and Distribution 81
6.3.1 Transition Path Time Distribution 82
6.3.2 Mean Transition Path Time 84
References 86
7 Sampling Transition Paths89
7.1 Dominant Paths and Instantons 92
7.1.1 Saddle-Point Method 92
7.1.2 The Euler-Lagrange Equation: Dominant Paths 92
7.1.3 Steepest Descent Method 96
7.1.4 Gradient Descent Method 97
7.2 Path Sampling 98
7.2.1 Metropolis Scheme 98
7.2.2 Langevin Scheme 99
7.3 Bridge and Conditioning 99
7.3.1 Free Particle 102
7.3.2 The Ornstein-Uhlenbeck Bridge 102
7.3.3 Exact Diagonalization 104
7.3.4 Cumulant Expansion 105
References 111
Appendix A: Gaussian Variables 111
Appendix B 113
8 The Rate of Conformational Change: Definition and Computation117
8.1 First-order Chemical Kinetics 117
8.2 Rate Coefficients from Microscopic Dynamics 119
8.2.1 Validity of First Order Kinetics 120
8.2.2 Mapping Continuous Trajectories onto Discrete Kinetics and Computing Exact Rates 123
8.2.3 Computing the Rate More Efficiently 126
8.2.4 Transmission Coefficient and Variational Transition State Theory 128
8.2.5 Harmonic Transition-State Theory 129
References 131
9 Zwanzig-Caldeiga-Leggett Model for Low-Dimensional Dynamics133
9.1 Low-Dimensional Models of Reaction Dynamics From a Microscopic Hamiltonian 133
9.2 Statistical Properties of the Noise and the Fluctuation-dissipation Theorem 137
9.2.1 Ensemble Approach 138
9.2.2 Single-Trajectory Approach 139
9.3 Time-Reversibility of the Langevin Equation 142
References 145
10 Escape from a Potential Well in the Case of Dynamics Obeying the Generalized Langevin Equation: General Solution Based on the Zwanzig-Caldeira-Leggett Hamiltonian147
10.1 Derivation of the Escape Rate 147
10.2 The Limit of Kramers Theory 150
10.3 Significance of Memory Effects 152
10.4 Applications of the Kramers Theory to Chemical Kinetics in Condensed Phases, Particularly in Biomolecular Systems 153
10.5 A Comment on the Use of the Term Free Energy in Application to Chemical Kinetics and Equilibrium 155
References 156
11 Diffusive Dynamics on a Multidimensional Energy Landscape157
11.1 Generalized Langevin Equation with Exponential Memory can be Derived from a 2D Markov Model 157
11.2 Theory of Multidimensional Barrier Crossing 161
11.3 Breakdown of the Langer Theory in the Case of Anisotropic Diffusion: the Berezhkovskii-Zitserman Case 167
References 171
12 Quantum Effects in Chemical Kinetics173
12.1 When is a Quantum Mechanical Description Necessary? 173
12.2 How Do the Laws of Quantum Mechanics Affect the Observed Transition Rates? 174
12.3 Semiclassical Approximation and the Deep Tunneling Regime 177
12.4 Path Integrals, Ring-Polymer Quantum Transition-State Theory, Instantons and Centroids 184
References 191
13 Computer Simulations of Molecular Kinetics: Foundation193
13.1 Computer Simulations: Statement of Goals 193
13.2 The Empirical Energy 195
13.3 Molecular States 197
13.4 Mean First Passage Time 199
13.5 Coarse Variables 199
13.6 Equilibrium, Stable, and Metastable States 200
References 202
14 The Master Equation as a Model for Transitions Between Macrostates203
References 211
15 Direct Calculation of Rate Coefficients with Computer Simulations213
15.1 Computer Simulations of Trajectories 213
15.2 Calculating Rate with Trajectories 219
References 221
16 A Simple Numerical Example of Rate Calculations223
References 231
17 Rare Events and Reaction Coordinates233
References 240
18 Celling241
References 252
19 An Example of the Use of Cells: Alanine Dipeptide255
References 257
Index 259
