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Master Equation for Markov Processes
Jul 2, 2024
Master Equation for Markov Processes
Introduction
Discussed the master equation for Markov processes.
Defined conditional probability density for the system being in state k at time t given it was in state j at time 0.
Equations are first-order coupled differential equations.
Transition rates (W) describe going from state l to state k (l
Master Equation Form
Written as:
[ \frac{d}{dt} p(k, t | j, 0) = \sum_{l=1}^{n} [W_{kl} p(l, t | j, 0) - W_{lk} p(k, t | j, 0)] ]
Constraint: l ≠ k
Initial condition: [ p(k, 0 | j) = \delta_{kj} ]
Vector and Matrix Representation
Represent as a column vector.
[ p(t) = \begin{pmatrix} p_1(t | j) \ p_2(t | j) \ \vdots\ \ p_n(t | j) \end{pmatrix} ]
Transition matrix W elements:
Off-diagonal: [ W_{kj} = W_{kl} , \text{(transition rates)} , \text{for} , k , \ne , j ]
Diagonal: [ W_{kk} = -\sum_{l \ne k} W_{lk} ]
Determinant of W is zero, W has real elements:
Off-diagonal elements: 0 or positive
Diagonal elements: negative
Special Cases and Detailed Balance
Important cases include detailed balance where each transition rate is pairwise equal.
[ W_{kl} p(l) = W_{lk} p(k) ]
Detailed balance often applies in thermodynamic equilibrium.
General stationary distribution and normalization.
[ \sum_{k=1}^{n} p(k) = 1 ]
Explicit Solution for Special Cases
Simple cases such as dichotomous Markov processes (two states):
Transition rates: λ1 (from state 1 to state 2) and λ2 (from state 2 to state 1).
Stationary distribution:
[ p_1 = \frac{\lambda_2}{\lambda_1 + \lambda_2} ]
[ p_2 = \frac{\lambda_1}{\lambda_1 + \lambda_2} ]
Average residence time: τ₁ and τ₂ related to transition rates.
[ \lambda_1 = \frac{1}{\tau_1} ]
[ \lambda_2 = \frac{1}{\tau_2} ]
Exponential Solution
General solution for p(t):
[ p(t) = e^{Wt} p(0) ]
Eigenvalues of W, rate of decay towards equilibrium determined via Gershgorin Disc Theorem.
Correlation Time
Defined as the harmonic mean of individual residence times:
[ \tau_c = \frac{2}{\lambda_1 + \lambda_2} = \frac{\tau_1 \tau_2}{\tau_1 + \tau_2} ]
Relates to how the process loses memory of its initial state.
Autocorrelation function expected to decay exponentially.
[ \langle\delta x(0) \delta x(t) \rangle \propto e^{-2\lambda t} ]
Summary
The master equation is foundational to understanding Markov processes and their long-term behavior.
The stationary distribution and transition rates are key to the system's equilibrium state.
Detailed balance simplifies solution finding in thermodynamic systems.
For dichotomous Markov processes, explicit solutions provide insight into dynamic behavior and correlation times.
Future discussion to detail exponential correlations and autocorrelation functions in Markov processes.
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