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Normal Mode Theory and Harmonic Potential Approximations |
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1 | (16) |
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1 | (1) |
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2 | (3) |
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5 | (6) |
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7 | (2) |
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Langevin and Brownian Modes |
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9 | (2) |
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Interpretation and Analysis of Normal Modes |
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11 | (4) |
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15 | (2) |
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16 | (1) |
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All-Atom Normal Mode Calculations of Large Molecular Systems Using Iterative Methods |
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17 | (24) |
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17 | (2) |
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19 | (2) |
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21 | (2) |
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Methods Based on the Rayleigh Quotient |
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21 | (1) |
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22 | (1) |
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23 | (1) |
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23 | (4) |
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24 | (1) |
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Iterative Procedure for Obtaining the NMs |
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24 | (1) |
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24 | (3) |
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27 | (6) |
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27 | (1) |
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Comparison between DIMB and the SM |
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28 | (1) |
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Utilization of DIMB with a Different Partition |
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29 | (1) |
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Coupling Between Backbone Collective Motions and Side-Chains |
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30 | (2) |
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32 | (1) |
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33 | (8) |
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Appendix A Detailed Description of the DIMB Method |
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34 | (1) |
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34 | (2) |
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Iterative Procedure for Obtaining the NMs |
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36 | (1) |
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36 | (5) |
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The Gaussian Network Model: Theory and Applications |
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41 | (24) |
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41 | (3) |
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Conformational Dynamics: A Bridge Between Structure and Function |
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43 | (1) |
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Functional Motions of Proteins Are Cooperative Fluctuations Near the Native State |
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43 | (1) |
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The Gaussian Network Model |
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44 | (5) |
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A Minimalist Model for Fluctuation Dynamics |
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44 | (1) |
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GNM Assumes Fluctuations Are Isotropic and Gaussian |
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44 | (2) |
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Statistical Mechanics Foundations of the GNM |
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46 | (2) |
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Influence of Local Packing Density |
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48 | (1) |
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49 | (10) |
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49 | (1) |
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GNM Mode Decomposition: Physical Meaning of Slow and Fast Modes |
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50 | (3) |
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What Is ANM? How Does GNM Differ from ANM? |
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53 | (2) |
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Applicability to Supramolecular Structures |
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55 | (3) |
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iGNM: A Database of GNM Results |
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58 | (1) |
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59 | (6) |
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61 | (4) |
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Normal Mode Analysis of Macromolecules: From Enzyme Active Sites to Molecular Machines |
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65 | (26) |
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65 | (1) |
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Basic Theories and Implementations |
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66 | (5) |
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NMA with Hybrid QM/MM Potentials |
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67 | (2) |
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Coarse-Grained NMA with Physical Potentials |
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69 | (2) |
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Illustrative Applications |
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71 | (12) |
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71 | (4) |
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Flexibility of Molecular Machines --- Comparison between BNM and ANM |
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75 | (1) |
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75 | (4) |
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The 30S and 50S Ribosomes |
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79 | (4) |
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Conclusions and Future Perspectives |
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83 | (8) |
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84 | (1) |
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84 | (7) |
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Functional Information from Slow Mode Shapes |
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91 | (20) |
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91 | (2) |
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Conformational Change of AdK Arising from NMA |
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93 | (10) |
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Standard Normal Mode Calculation |
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93 | (1) |
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Comparison with the Conformational Change |
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94 | (1) |
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Effective Number of Modes Required for the Description |
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95 | (1) |
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96 | (2) |
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98 | (3) |
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Description of the Conformational Change with Approximate Modes |
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101 | (2) |
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Conformational Change of DHFR and NMA |
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103 | (2) |
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105 | (1) |
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106 | (5) |
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106 | (5) |
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Unveiling Molecular Mechanisms of Biological Functions in Large Macromolecular Assemblies Using Elastic Network Normal Mode Analysis |
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111 | (26) |
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112 | (1) |
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113 | (6) |
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113 | (1) |
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Multi-Scale Energy Functions Using Elastic Networks |
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114 | (1) |
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Rotation-Translation Block Method |
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115 | (2) |
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Multi-Scale NMA Using Elastic Network Hamiltonians and the RTB Method |
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117 | (1) |
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Mapping the Pathway of Conformational Change Using NMA |
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117 | (1) |
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Linear Interpolation between Endpoints Using Normal Mode Directions |
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117 | (1) |
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Nonlinear/Iterative Approach |
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118 | (1) |
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119 | (14) |
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Unveiling Molecular Mechanisms of Conformational Changes of Large Macromolecular Assemblies |
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120 | (1) |
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The Mechanism and Pathway of pH Induced Swelling in Cowpea Chlorotic Mottle Virus |
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120 | (3) |
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Dynamic Reorganization of the Functionally Active 70S Ribosome |
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123 | (3) |
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Myosin II ATPase Inhibition |
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126 | (2) |
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Exploration of Global Distortions and Interpretation of Low-Resolution Structural Information |
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128 | (1) |
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Global Distortions of Biological Molecules from Low-Resolution Structural Information |
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128 | (1) |
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Flexible Fitting of Atomic Structures into Low-Resolution Electron Density Maps |
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129 | (4) |
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133 | (4) |
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133 | (1) |
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134 | (3) |
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Applications of Normal Mode Analysis in Structural Refinement of Supramolecular Complexes |
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137 | (18) |
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137 | (1) |
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138 | (2) |
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138 | (1) |
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139 | (1) |
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Structural Refinement in Cryo-EM Measurement |
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140 | (6) |
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NMA Based on Low-Resolution Density Maps |
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140 | (4) |
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QEDM-Assisted Cryo-EM Structural Refinement |
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144 | (2) |
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Structural Refinement in Fiber Diffraction |
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146 | (9) |
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NMA at Length Scales of Several Microns |
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146 | (2) |
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Fiber Diffraction Refinement Based on Long-Range Normal Modes |
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148 | (2) |
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150 | (1) |
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151 | (4) |
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Normal Mode Analysis in Studying Protein Motions with X-Ray Crystallography |
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155 | (16) |
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155 | (4) |
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Comparison of Theory and Diffraction Experiment |
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159 | (2) |
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Effect of Displacements on the Bragg Peaks |
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161 | (3) |
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Normal Mode Predictions of X-Ray Diffuse Scattering |
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163 | (1) |
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Complete Refinement Strategies |
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164 | (7) |
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165 | (1) |
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165 | (6) |
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Optimizing the Parameters of the Gaussian Network Model for ATP-Binding Proteins |
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171 | (16) |
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171 | (1) |
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172 | (4) |
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172 | (1) |
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173 | (2) |
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175 | (1) |
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176 | (1) |
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176 | (9) |
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176 | (1) |
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Pair Distribution Functions |
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177 | (1) |
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178 | (1) |
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Correlation Coefficients at Different Cutoff Distances and Spring Constants |
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178 | (2) |
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Cases of Highest Correlations |
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180 | (1) |
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Mean-Square Fluctuation Predictions for the Cases That Show Highest Correlations |
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181 | (1) |
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Comparison of Fluctuations for Different Spring Constants |
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181 | (4) |
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Comparison of Fluctuations at Different Cutoff Distances |
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185 | (1) |
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185 | (2) |
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185 | (2) |
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Effects of Sequence, Cyclization, and Superhelical Stress on the Internal Motions of DNA |
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187 | (26) |
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188 | (1) |
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189 | (4) |
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189 | (1) |
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190 | (1) |
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191 | (1) |
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192 | (1) |
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Imposed Superhelical Stress |
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192 | (1) |
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193 | (2) |
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193 | (1) |
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193 | (1) |
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194 | (1) |
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Role of Intrinsic Structure |
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195 | (5) |
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Intrinsic Bending and Single-Molecule Stretching |
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195 | (2) |
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Intrinsic Curvature and DNA Ring Puckering |
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197 | (1) |
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Intrinsic Curvature and Enzyme Cutting Patterns |
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198 | (2) |
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Role of Sequence-Dependent Deformability |
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200 | (2) |
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Dimer Deformability and Large-Scale Anisotropy of Linear DNA |
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200 | (1) |
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Dimer Deformability and Rotational Positioning of Circular DNA |
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201 | (1) |
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Role of Conformational Coupling |
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202 | (4) |
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Roll-Slide Interdependence and Supercoiling of Circular DNA |
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202 | (2) |
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Twist-Rise Coupling and Overstretching of Linear DNA |
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204 | (2) |
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206 | (7) |
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207 | (1) |
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207 | (6) |
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Symmetry in Normal Mode Analysis of Icosahedral Viruses |
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213 | (20) |
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213 | (2) |
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215 | (4) |
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215 | (3) |
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218 | (1) |
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219 | (9) |
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219 | (1) |
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220 | (7) |
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227 | (1) |
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228 | (5) |
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230 | (1) |
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230 | (3) |
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Extension of the Normal Mode Concept: Principal Component Analysis, Jumping-Among-Minima Model, and Their Applications to Experimental Data Analysis |
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233 | (20) |
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233 | (1) |
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Collective-Mode Description of Protein Dynamics |
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234 | (1) |
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Principal Component Analysis |
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235 | (3) |
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238 | (1) |
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Conservation and Convergence of Collective Variables |
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239 | (2) |
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Anharmonicity of Energy Landscape and JAM Model |
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241 | (2) |
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Application of JAM Concept |
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243 | (3) |
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Application of the Normal Mode Concept to the Dynamics Crystallographic Refinement |
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246 | (1) |
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247 | (2) |
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249 | (4) |
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249 | (4) |
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Imaginary-Frequency, Unstable Instantaneous Normal Modes, the Potential Energy Landscape, and Diffusion in Liquids |
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253 | (28) |
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254 | (2) |
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Unstable Modes and Diffusion |
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256 | (14) |
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Statistical Mechanics on the PEL |
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257 | (1) |
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The Partition Function and the Im --- ω Density of States |
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257 | (3) |
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260 | (1) |
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The Functional Form of the Density of States |
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261 | (1) |
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262 | (4) |
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266 | (1) |
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The Fraction of Unstable Frequencies, Dynamics, and Tc |
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267 | (2) |
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The Configurational Entropy Sc |
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269 | (1) |
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Diffusive and Nondiffusive Unstable Modes |
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270 | (5) |
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Potential Energy Profile Based Methods |
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271 | (1) |
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272 | (1) |
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272 | (1) |
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273 | (1) |
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273 | (2) |
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275 | (6) |
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276 | (1) |
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276 | (5) |
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Driven Molecular Dynamics for Normal Modes of Biomolecules without the Hessian, and Beyond |
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281 | (20) |
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281 | (2) |
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Driven Molecular Dynamics |
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283 | (2) |
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283 | (2) |
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Computational Implementation |
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285 | (1) |
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285 | (11) |
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The Harmonic Limit: Trp-Cage |
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285 | (1) |
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286 | (1) |
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Spectral Density and Resolution |
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286 | (2) |
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288 | (2) |
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Correlation of Atomic Motion |
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290 | (1) |
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291 | (1) |
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Beyond the Harmonic Limit: Dialanine |
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292 | (1) |
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Anharmonic Driving of Interatomic Distances |
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293 | (1) |
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Electric Dipole-Driven Dynamics |
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294 | (2) |
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296 | (5) |
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298 | (1) |
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298 | (3) |
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Probing Vibrational Energy Relaxation in Proteins Using Normal Modes |
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301 | (24) |
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301 | (1) |
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302 | (1) |
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303 | (6) |
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304 | (1) |
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Quantum Correction Factor |
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305 | (1) |
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NM Calculations for Cyt c |
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306 | (1) |
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Application to VER of the CD Bond in Cyt c |
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307 | (1) |
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Fluctuation of the CD Bond Frequency |
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308 | (1) |
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309 | (6) |
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Reduced Model for a Protein |
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310 | (1) |
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311 | (1) |
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Third-Order Coupling Elements |
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312 | (1) |
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313 | (2) |
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315 | (1) |
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315 | (3) |
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Comparison with Experiment |
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315 | (1) |
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Validity of Fermi's Golden Rule |
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316 | (1) |
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Higher-Order Coupling Terms |
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317 | (1) |
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318 | (7) |
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320 | (1) |
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320 | (5) |
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Anharmonic Decay of Vibrational States in Proteins |
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325 | (24) |
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325 | (3) |
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Computation of Vibrational Lifetimes |
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328 | (2) |
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Vibrational Energy Transfer in Proteins |
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330 | (9) |
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330 | (5) |
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Photoactive Yellow Protein |
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335 | (4) |
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339 | (10) |
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341 | (1) |
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Appendix: Force Field for Chromophore |
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342 | (1) |
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343 | (6) |
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Collective Coordinate Approaches to Extended Conformational Sampling |
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349 | (18) |
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349 | (1) |
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Extended Sampling Methods |
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350 | (9) |
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Principal Component Analysis |
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350 | (2) |
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352 | (2) |
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354 | (1) |
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Principal Component Restraints |
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354 | (5) |
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359 | (4) |
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Characterization of the Free Energy Surface Around the Native Structure |
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359 | (1) |
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Rapid Conformational Sampling |
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359 | (2) |
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Large Conformational Motions: Allosteric Transitions, Unfolding, Folding |
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361 | (2) |
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363 | (4) |
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363 | (1) |
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363 | (4) |
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Using Collective Coordinates to Guide Conformational Sampling in Atomic Simulations |
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367 | (22) |
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368 | (2) |
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Biomolecular Simulations and Enhanced Conformation Sampling |
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368 | (1) |
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A Qualitative Picture of the Conformational Energy Landscape |
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368 | (1) |
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Objectives and Basic Strategies for Enhanced Conformation Sampling |
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369 | (1) |
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Using Collective Coordinates for Enhanced Conformation Sampling |
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370 | (2) |
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Collective Coordinate Descriptions of Protein Dynamics |
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370 | (1) |
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Enhanced Sampling Methods Employing Collective Coordinates |
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371 | (1) |
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The Amplified Collective Motion Method |
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372 | (6) |
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The Weak Coupling Method for Constant Temperature MD Simulations |
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372 | (1) |
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373 | (2) |
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Using ANM to Guide Atomic Simulations in the ACM Scheme |
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375 | (1) |
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The Amplified Collective Motion-Assisted Minimum Escaping (ACM-AME) Scheme |
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376 | (2) |
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378 | (6) |
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Interdomain Motions of Bacteriophage T4 Lysozyme |
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378 | (2) |
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Folding of an S-Peptide Analog |
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380 | (3) |
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ACM-AME Sampling of Peptide Conformations |
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383 | (1) |
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384 | (5) |
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385 | (1) |
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385 | (4) |
Index |
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389 | |