LINEAR-ALGEBRA Β· Interactive Practice | Unit 23 Β· Video 2
| Formula | Name | Description |
|---|---|---|
| Markov iteration | One time step of the chain | |
| Spectral master formula | Powers of in the eigenvector basis | |
| for | Markov spectrum | Always true for column-stochastic |
| as | Steady state | Only the direction survives |
Each step fraction leaves City A and fraction leaves City B; run the chain forward and watch the split settle.
π‘ For the steady state is β fixed by the rates alone, never by the start.
Every non-dominant term decays like ; the closer sits to 1, the slower the chain forgets.
π‘ The steps needed to shrink to 1% is the chain's mixing time; the ratio that sets it is the mixing rate.
Six different starting splits, all on the line β every trajectory slides to the same steady-state point.
Question 1
For any column-stochastic Markov matrix , what is the largest eigenvalue ?
β Correct! Every column-stochastic matrix has β guaranteed by the columns summing to 1.
β Not quite. The columns-sum-to-1 property forces a specific eigenvalue. Think about what equals.
Solution:
Every column-stochastic matrix has columns summing to 1. This means the all-ones row vector satisfies , so is a left eigenvector with eigenvalue . Since and share eigenvalues, is also an eigenvalue of .
Combined with the PerronβFrobenius bound for all eigenvalues of a stochastic matrix, we conclude:
Question 2
A Markov chain has eigenvalues , , and . Approximately how many steps are needed for the non-dominant components to decay by a factor of about 100 (i.e., )?
β Correct! . The slowest-decaying eigenvalue sets the mixing time.
β Not quite. Convergence is controlled by the second-largest eigenvalue. Solve .
Solution:
The convergence rate is governed by the second-largest eigenvalue magnitude, . We want:
Taking logs: .
So about 90 steps. Note that decays much faster ( is astronomically tiny), so it's irrelevant β the slowest non-dominant eigenvalue dominates the mixing time.
Question 3
True or False: For a (well-behaved) Markov chain, the steady state depends on the starting distribution .
β Correct! The steady state is determined by the matrix's eigenvector, and the probability constraint pins β independent of .
β Not quite. Look back at Visualization 3: six different starting splits all flowed to the same red star.
Solution:
The master formula gives . As , only the first term survives, so:
The direction is fixed by the matrix β it does not depend on at all. The scalar does depend on in principle, but for any probability vector (entries non-negative, summing to 1), the constraint that also sums to 1 pins down uniquely.
Result: every probability starting distribution converges to the same steady state. The chain forgets where it began.
(Caveat: this assumes has multiplicity one and the chain is irreducible/aperiodic β the well-behaved case.)
Question 4
Consider the column-stochastic matrix
What is the steady-state distribution (the eigenvector for , normalized so its entries sum to 1)?
β Correct! Solving and normalizing gives .
β Not quite. would only be the steady state if the matrix were symmetric (e.g., ). Here .
β Not quite. Reading the diagonal isn't the same as solving . Set up the eigenvalue equation.
β Not quite. You may have swapped the components. Solve carefully.
Solution:
We need , i.e., :
The first row gives , so , or .
Normalizing so the entries sum to 1:
Shortcut for 2Γ2 column-stochastic : steady state is . Here , , giving .
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