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Theory of Stochastic Processes
A.A. 2024/25
Aggiornamento del 08.01.25
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Motivation
- Brownian Motion: Einstein and Langevin description.
- Birth-Death processes: Master equation.
- Shot Noise: Stochastic Differential Equation.
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Stochastic Processes
- Definitions.
- Bernoulli Trials.
- Markov Processes.
- The Chapman-Kolmogorov equation.
- Continuous Markov processes; examples: Brownian motion and Cauchy process.
- Differential Chapman-Kolmogorov equation.
- The master equation: jump processes.
- The Liouville equation: deterministic processes.
- The Fokker-Planck equation: diffusive processes.
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Fokker-Planck Equation
- Backward differential Chapman-Kolmogorov equation.
- Forward Kramers-Moyal equation.
- Stationary and homogeneous Markov Processes.
- The Wiener Process.
- The Ornstein-Uhlembeck proceess.
- The method of characteristics for quasilinear partial differential equations.
- Probability current and boundary conditions for the Fokker-Planck equation.
- Stationary solution for the one-dimensional homegeneous Fokker-Planck equation:
Potential solutions.
- Stationary solution in a gravitational field.
- Stationary solution of the Ornstein-Uhlembeck process.
- Stationary solution for the Brownian motion.
- The eigenvalue method: Wiener process with absorbing and reflectin barriers.
- First Passage Time for homogeneous processes.
- Escape over a potential barrier, the Arrhenius formula.
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Stochastic Differential Equations
- The Langevin equation and the Wiener process.
- The stochastic integration: the Ito Integral.
- Nonanticipating functions.
dW(t)2 and dW(t)2+N .
- The Stratonovich Integral.
- The Ito differentiation rule.
- The Dirac delta function and the Heaviside theta function.
- Numerical integration of SDE: Stochastic second order Runge-Kutta Algorithm.
- The Ito formula.
- Ito SDE and Fokker-Planck equation.
- Ito and Stratonovich SDE.
- Stratonovich SDE and Fokker-Planck equation.
- Example: SDE with linear multiplicative noise.
- Example: Linear oscillator with random frequency.
- Formalismo di Martin-Siggia-Rose
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Path Integral Methods for Stochastic Differential Equations
- Path Integral formulation for additive white noise Langevin equations.
- The Martin-Siggia-Rose-Janssen-de Domicis (MSRJD) Action.
- The Onsager-Machlup-Graham-Bausch-Wegner (OMGBW) Action.
- Derivation of the Fokker-Planck equation from the path integral.
- Response functions and response fields.
- Quadratic MSRJD action.
- Example: The one dimensional Ornstein-Uhlembeck process.
- Path Integral formulation for multiplicative white noise Langevin equations.
- From Path Integral to Fokker-Planck equation for multiplicative white noise processes:
state dependent diffusion.
- Thermodynamic equilibrium conditions for multiplicative white noise processes.
- Fluctuation-Dissipation Theorem for additive white noise processes.
- Detailed Balance condition.
- Fluctuation-Dissipation Theorem for multiplicative white noise processes.
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Dynamical Field Theory
- The Novikov and Wick theorems.
- Perturbation theory in the nonlinearity (interaction).
- Perturbative evaluation of (equilibrium) two points functions.
- The Dyson equation.
- The Dyson equation for the zero-dimensional
λϕ4 model: first order calculation.
- Perturbation theory in the non linearity with non zero external field.
- Dynamical Effective potential
Γ[φ,φ̂] .
- Dynamical Effective potential for the Ornstein-Uhlembeck process.
- Loop expansion of the Dynamical Effective potential.
- Dynamical Effective potential for the zero-dimensional
λϕ4 model: zero and one loop calculation.
- Conditional Probability Function: the
φ̂ ≠ 0 solution.
- Dynamical Effective Potential and Conditional Probability Function.
- Arrhenius Law.
- Quantum averages over the Close Time Path (CTP) contour.
- Bosonic Coherent States.
- CTP calculation of Z[0] for
the bosonic system Ĥ = ω0 b̂+ b̂.
- CTP Green function for
the bosonic system Ĥ = ω0 b̂+ b̂.
- The Keldysh formalism.
- Quantum Harmonic Oscillator.
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Dynamical Field Theory for disordered systems.
- Quenched disorder average in statics and dynamics.
- Random non-symmetric two-body interaction neural network model:
averaged dynamical generating function.
- The spherical p-spin and 2+p-spin spin-glass models: averaged dynamical generating
function and effective dynamics.
- Equilibrium dynamics of the spherical 2+p-spin spin-glass models.
- Ergodic dynamics of the 2+3-spin spin-glass model:
critical slowing down and continuous transition.
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- Ergodic dynamics of the 2+3-spin spin-glass model:
dynamical arrest and discontinuous transition.
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- Non-ergodic dynamcis of the 2+3-spin spin-glass model:
two-steps relaxation, dynamical marginal condition and 1RSB phase.
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- Path-Integral approach to a fully connected neural network model with
random independent asymmetric couplings.
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Argomenti facoltativi ai fini dell'esame.
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