Preface |
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vii | |
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*Introduction and outline |
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1 | (14) |
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Hamiltonian dynamical systems approach to nonequilibrium statistical mechanics |
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2 | (5) |
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Thermostated dynamical systems approach to nonequilibrium statistical mechanics |
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7 | (4) |
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The red thread through this book |
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11 | (4) |
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Part 1: Fractal transport coefficients |
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15 | (148) |
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17 | (12) |
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A simple model for deterministic diffusion |
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17 | (5) |
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A parameter-dependent fractal diffusion coefficient |
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22 | (6) |
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28 | (1) |
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Deterministic drift-diffusion |
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29 | (26) |
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Drift-diffusion model: mathematical definition |
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29 | (3) |
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+Calculating deterministic drift and diffusion coefficients |
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32 | (8) |
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Twisted eigenstate method |
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33 | (4) |
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Transition matrix methods |
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37 | (2) |
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Numerical comparison of the different methods |
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39 | (1) |
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40 | (9) |
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Simple maps as deterministic ratchets |
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49 | (5) |
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54 | (1) |
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Deterministic reaction-diffusion |
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55 | (28) |
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A reactive-diffusive multibaker map |
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55 | (7) |
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Deterministic models of reaction-diffusion |
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56 | (4) |
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The Frobenius-Perron operator |
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60 | (2) |
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62 | (8) |
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+Diffusive modes of the dyadic multibaker |
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62 | (2) |
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The parameter-dependent diffusion coefficient |
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64 | (6) |
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70 | (11) |
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+Reactive modes of the dyadic multibaker |
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70 | (5) |
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The parameter-dependent reaction rate |
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75 | (6) |
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81 | (2) |
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Deterministic diffusion and random perturbations |
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83 | (16) |
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Disordered dynamical systems |
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83 | (6) |
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89 | (9) |
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98 | (1) |
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From normal to anomalous diffusion |
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99 | (22) |
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Deterministic diffusion and bifurcations |
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99 | (8) |
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Anomalous diffusion in intermittent maps |
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107 | (12) |
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119 | (2) |
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From diffusive maps to Hamiltonian particle billiards |
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121 | (16) |
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Correlated random walks in maps |
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121 | (7) |
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Correlated random walks in billiards |
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128 | (6) |
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134 | (3) |
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Designing billiards with irregular transport coefficients |
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137 | (16) |
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Diffusion in the flower-shaped billiard |
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137 | (4) |
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+Random and correlated random walks |
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141 | (7) |
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Diffusion in porous solids |
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148 | (2) |
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150 | (3) |
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Deterministic diffusion of granular particles |
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153 | (10) |
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Resonances and diffusion in the bouncing ball billiard |
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153 | (4) |
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+Diffusion by correlated random walks |
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157 | (3) |
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160 | (1) |
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161 | (2) |
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Part 2: Thermostated dynamical systems |
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163 | (154) |
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Motivation: coupling a system to a thermal reservoir |
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165 | (20) |
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165 | (2) |
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*Modeling thermal reservoirs: the Langevin equation |
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167 | (6) |
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Equilibrium velocity distributions for thermostated systems |
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173 | (6) |
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Applying thermostats: the periodic Lorentz gas |
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179 | (4) |
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183 | (2) |
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185 | (20) |
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Construction of the Gaussian thermostat |
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185 | (4) |
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Chaos and transport in Gaussian thermostated systems |
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189 | (13) |
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Phase space contraction and entropy production |
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189 | (1) |
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Lyapunov exponents and transport coefficients |
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190 | (3) |
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Nonequilibrium fractal attractors |
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193 | (5) |
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198 | (4) |
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202 | (3) |
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The Nose-Hoover thermostat |
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205 | (26) |
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The dissipative Liouville equation |
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205 | (3) |
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Construction of the Nose-Hoover thermostat |
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208 | (5) |
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208 | (2) |
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Physics of this thermostat |
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210 | (3) |
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Properties of the Nose-Hoover thermostat |
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213 | (9) |
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213 | (2) |
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+Generalized Hamiltonian formalism |
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215 | (3) |
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218 | (4) |
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+Subtleties of Nose-Hoover dynamics |
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222 | (5) |
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Necessary conditions and generalizations |
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222 | (4) |
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Thermal reservoirs in nonequilibrium |
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226 | (1) |
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227 | (4) |
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Universalities in Gaussian and Nose-Hoover dynamics? |
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231 | (26) |
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Non-Hamiltonian nonequilibrium steady states |
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231 | (4) |
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Phase space contraction and entropy production |
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235 | (5) |
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Transport coefficients and dynamical systems quantities |
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240 | (7) |
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Fractal attractors for nonequilibrium steady states |
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247 | (4) |
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Nonlinear response in the driven periodic Lorentz gas |
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251 | (2) |
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253 | (4) |
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Gaussian and Nose-Hoover thermostats revisited |
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257 | (12) |
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Non-ideal Gaussian thermostat |
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257 | (4) |
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Non-ideal Nose-Hoover thermostat |
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261 | (3) |
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+Further alternative thermostats |
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264 | (2) |
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266 | (3) |
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Stochastic and deterministic boundary thermostats |
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269 | (34) |
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Stochastic boundary thermostats |
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270 | (1) |
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Deterministic boundary thermostats |
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271 | (2) |
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+Boundary thermostats from first principles |
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273 | (6) |
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Deterministic boundary thermostats for the driven periodic Lorentz gas |
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279 | (8) |
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Phase space contraction and entropy production |
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280 | (3) |
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Attractors, bifurcations and conductivity |
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283 | (3) |
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286 | (1) |
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Hard disk fluid under shear and heat flow |
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287 | (13) |
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Homogeneously and inhomogeneously driven shear and heat flows |
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288 | (3) |
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Shear and heat flows thermostated by deterministic scattering |
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291 | (9) |
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300 | (3) |
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Active Brownian particles and Nose-Hoover dynamics |
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303 | (14) |
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Brownian motion of migrating cells? |
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304 | (2) |
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+Moving biological entities as active Brownian particles |
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306 | (2) |
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+Bimodal velocity distributions and Nose-Hoover dynamics |
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308 | (6) |
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314 | (3) |
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Part 3: Outlook and conclusions |
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317 | (64) |
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Further topics in chaotic transport theory |
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319 | (48) |
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320 | (11) |
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Entropy fluctuation in nonequilibrium steady states |
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320 | (1) |
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The Gallavotti-Cohen fluctuation theorem |
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321 | (6) |
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The Evans-Searles fluctuation theorem |
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327 | (1) |
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Jarzynski work relation and Crooks relation |
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328 | (3) |
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331 | (6) |
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337 | (10) |
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338 | (2) |
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Heat conduction in anharmonic chaotic chains |
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340 | (4) |
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Heat conduction in chaotic particle billiards |
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344 | (3) |
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347 | (17) |
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Microscopic chaos and diffusion? |
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348 | (4) |
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Polygonal billiard channels |
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352 | (12) |
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364 | (3) |
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367 | (14) |
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Microscopic chaos and nonequilibrium statistical mechanics: the big picture |
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367 | (4) |
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Assessment of the main results |
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371 | (5) |
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Existence of fractal transport coefficients |
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371 | (3) |
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Universalities in thermostated dynamical systems? |
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374 | (2) |
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376 | (5) |
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Fractal transport coefficients |
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377 | (2) |
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Thermostated dynamical systems |
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379 | (1) |
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380 | (1) |
Bibliography |
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381 | (54) |
Index |
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435 | |