Discrete-time Markov chains move at fixed ticks; the Poisson process moves in continuous time but only ever counts upward by 1. This topic's opening lesson merges the two ideas: a continuous-time Markov chain (CTMC) is a process that, like a discrete chain, can jump between arbitrary states, but does so at random continuous-time instants governed by exponential holding times — combining the Markov chain's state-dependent transition structure with the Poisson process's memoryless timing. The generator matrix , built from state-dependent jump rates, plays exactly the role the transition matrix played in discrete time, and the embedded jump chain shows every CTMC can be built from an ordinary discrete chain plus a sequence of independent exponential clocks.
Learning objectives. By the end of this note you should be able to:
- state the continuous-time Markov property and define the jump rates ;
- construct the generator matrix from a verbal description of a system;
- describe the embedded-jump-chain construction of a CTMC and simulate it;
- recognise the explosion phenomenon and state uniformization as a simulation tool.
In this lesson
- Definition and jump rates
- Constructing the chain from its rates
- Explosion
- Uniformization
The full lesson, with worked examples and exercise solutions, is for members.
Read the full lessonNew to SelfMadeQuant.com? See membership options or explore the curriculum.