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Preface | p. V |
Acknowledgements | p. VII |
Acronyms | p. XI |
Symbols | p. XIII |
Introduction | p. 1 |
Theory and phenomenology of glasses | p. 15 |
Processes, timescales and transitions | p. 15 |
Dynamical glass transition | p. 17 |
Thermal glass transition | p. 19 |
Strong and fragile glass formers | p. 23 |
Aging | p. 26 |
Time sector separation | p. 28 |
Configurational entropy | p. 29 |
Kauzmann paradox | p. 30 |
Static phase transition and Kauzmann temperature | p. 31 |
"Classic" versus "modern" configurational entropy | p. 31 |
An intrinsically dynamic "state" function | p. 33 |
Adam-Gibbs entropic theory | p. 34 |
Absence of flow in cathedral glasses | p. 37 |
Fragility index | p. 38 |
Kovacs effect | p. 39 |
Two temperature thermodynamics | p. 43 |
Elements of thermodynamics | p. 46 |
First law and second law | p. 46 |
Clausius-Clapeyron relation | p. 47 |
Maxwell relation | p. 48 |
Keesom-Ehrenfest relations and Prigogine-Defay ratio | p. 48 |
Fictive temperature | p. 50 |
Two temperature thermodynamics | p. 53 |
Two temperature thermodynamics for glassy systems | p. 55 |
Laws of thermodynamics for off-equilibrium systems | p. 56 |
Maxwell relation for aging systems | p. 58 |
Generalized Clausius-Clapeyron relation | p. 59 |
Keesom-Ehrenfest relations and Prigogine-Defay ratio out of equilibrium | p. 60 |
Laws of thermodynamics for glassy magnets | p. 64 |
Effective temperature in thermal cycles | p. 65 |
Fluctuation formula and effective temperatures | p. 70 |
Fluctuation and dissipation out of equilibrium | p. 72 |
Fluctuation-dissipation ratio | p. 74 |
Limits to the role of FDR as a temperature | p. 81 |
Direct measurement of the effective temperature | p. 83 |
Asymptotic solution in nonlinear cooling | p. 87 |
Exactly solvable models for the glassy state | p. 89 |
Harmonic oscillator model | p. 91 |
Analytically solvable Monte Carlo dynamics | p. 92 |
Parallel Monte Carlo versus Langevin dynamics | p. 96 |
Kinetic models with separation of timescales | p. 99 |
Statics and phase space constraint | p. 101 |
Parallel Monte Carlo dynamics of the HOSS model: equations of motion | p. 104 |
Dynamics of the strong glass model | p. 106 |
Dynamics of the fragile glass model | p. 109 |
Adam-Gibbs relation in the HOSS model | p. 115 |
Out-of-equilibrium thermodynamics | p. 116 |
Quasi-static approach | p. 116 |
Effective temperature from generalized laws | p. 118 |
Dynamic transition rate and effective temperature | p. 120 |
FDR and effective temperature | p. 123 |
Heat flow of [alpha] processes | p. 131 |
Effective temperature from a fluctuation formula | p. 131 |
Below the Kauzmann transition | p. 132 |
Instantaneous relaxation time | p. 134 |
Kovacs effect: limits of two temperature thermodynamics | p. 135 |
Analytical solution in the long-time regime | p. 138 |
Effective temperature and effective field | p. 140 |
Measuring effective temperature in HO models | p. 142 |
Heat flux between off-equilibrium systems | p. 144 |
Mode-dependent effective temperature | p. 146 |
Quasi-static effective temperature | p. 148 |
Mode-dependent fluctuation-dissipation ratio | p. 149 |
Transition rate effective temperature | p. 150 |
HOSS equations of motion for one-time variables | p. 152 |
Strong glass | p. 152 |
Fragile glass | p. 152 |
Analytic expressions for the Kovacs effect | p. 157 |
Monte Carlo integrals in one- and two-time dynamics | p. 158 |
Coefficients of the two-time variables equations | p. 160 |
Aging urn models | p. 163 |
The backgammon model | p. 166 |
Equilibrium thermodynamics | p. 167 |
Dynamics | p. 170 |
Adiabatic approximation and effective temperature | p. 174 |
Entropic barriers and a microcanonic derivation of the equation of motion | p. 178 |
Backgammon random walker | p. 179 |
Two-time dynamics and FDR effective temperature | p. 181 |
Effective temperature(s) in the backgammon model | p. 184 |
A model for collective modes | p. 185 |
Observables and equilibrium | p. 187 |
Dynamics of the disordered backgammon model | p. 190 |
Relaxational spectrum in equilibrium | p. 196 |
Specific examples of continuous energy distribution | p. 197 |
A method to determine the threshold energy scale | p. 201 |
Occupation probability density equations | p. 203 |
Ansatz for the adiabatic approximation | p. 205 |
Approach to equilibrium of occupation densities | p. 207 |
Probability distribution of proposed energy updates | p. 208 |
Glassiness in a directed polymer model | p. 211 |
The directed polymer model | p. 212 |
Disordered situation and Lifshitz-Griffiths singularities | p. 213 |
Static phase diagram | p. 216 |
Dual view in temperature | p. 218 |
Directed polymer dynamics | p. 219 |
Cooling and heating setups | p. 223 |
Poincare recurrence time | p. 223 |
Potential energy landscape approach | p. 225 |
Potential energy landscape | p. 228 |
Steepest descent | p. 229 |
Features of the PEL description borrowed from vitreous properties | p. 231 |
Inter- and intra-basins transitions: scales separation | p. 232 |
Inherent structures distribution: formal treatment | p. 233 |
Harmonic approximation | p. 236 |
Thermodynamics in supercooled liquids | p. 237 |
Inherent structure pressure | p. 237 |
Random energy model and Gaussian approximation | p. 239 |
Equation of state | p. 241 |
IS equation of State | p. 243 |
The solid amorphous phase | p. 244 |
PEL effective temperature from direct comparison to the aging dynamics | p. 245 |
PEL effective temperature and pressure in the two temperature thermodynamic framework | p. 246 |
The pressure in glasses | p. 249 |
Fragility in the PEL | p. 251 |
PEL approach to the random orthogonal model | p. 253 |
Effective temperature in the ROM | p. 254 |
PEL approach to the harmonic oscillator models | p. 256 |
PEL effective temperature in the HOSS model | p. 259 |
Quasi-static definition of IS effective temperature | p. 261 |
Many-body glassy models | p. 264 |
Soft spheres | p. 265 |
Lennard-Jones many-body interaction potential | p. 266 |
Lewis-Wahnstrom model for orthoterphenyl | p. 267 |
Simple point charge extended model for water | p. 268 |
Theories of the glassy state | p. 269 |
Mode-coupling theory | p. 269 |
Replica theory for glasses with quenched disorder | p. 274 |
The random energy model | p. 275 |
The p-spin model | p. 276 |
Complexity | p. 279 |
Mean-field scenario | p. 281 |
Glass models without quenched disorder: clone theory | p. 283 |
Equilibrium thermodynamics of the cloned m-liquid | p. 283 |
Analytic tools and specific behaviors in cloned glasses | p. 285 |
Effective temperature for the cloned molecular liquid | p. 287 |
Frustration limited domain theory | p. 289 |
Geometric frustration | p. 289 |
Avoided critical point | p. 291 |
Critical assessment of the approach | p. 294 |
Heuristic scaling arguments | p. 297 |
Random first order transition theory | p. 298 |
Adam-Gibbs theory, revisited | p. 300 |
Entropic driven "nucleation" and mosaic state | p. 301 |
Density functional for the RFOT theory | p. 305 |
Beyond entropic driving I: droplet partition function | p. 311 |
Beyond entropic driving II: library of local states | p. 315 |
Bibliography | p. 319 |
Index | p. 339 |
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