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Period two on a bipartite graph
Example
Let be an at most countable simple undirected graph that is connected, locally finite, bipartite with , and has no isolated vertices. For , write and . Define simple random walk by Then every vertex has period .
Facts & Assumptions
Given: The graph and transition matrix specified above. Local finiteness and the absence of isolated vertices mean for every .
The -step probabilities satisfy and . (Transition matrices and n-step probabilities)
For , . (Matrix Chapman–Kolmogorov equations)
States communicate when each is accessible from the other, and means for some . (Accessibility, communication, and irreducibility)
, and, when it is nonempty, is the greatest positive integer dividing every element of . (Period of a state)
If and communicate, then . (Period is constant on communicating classes)
Proof
Proof technique: use bipartite parity and a two-step backtrack at one vertex, then transfer the period across the connected graph.
If , there is no vertex to check. Otherwise fix . Every degree is finite and positive, so the displayed transition probabilities give a stochastic row at each vertex and are positive exactly on graph edges.
Let . Induction on using [F1] and [F2] shows that only for when is even and for when is odd: the base row is the identity row, and in the induction step Chapman–Kolmogorov together with the fact that every positive one-step transition crosses the bipartition flips the support side. Therefore for every odd , so every element of is even.
Since is not isolated, choose a neighbor . Undirectedness gives and . The case of [F2] yields , so .
By [F4], the positive return set at contains and consists only of even integers. Thus divides every return time, while every common positive divisor must divide the member ; hence the greatest such divisor is .
Fix any . Connectedness gives a finite edge path . If , repeated application of [F2] gives ; if , [F1] gives . Reversing the path gives positive accessibility from to as well. Thus and communicate by [F3], and [F5] yields . Since was arbitrary, every state has period two.
The empty graph has no vertices; a one-vertex graph would have an isolated vertex and is excluded. Degree-one vertices are allowed, and their immediate backtrack still gives a positive two-step return. The zero transitions within each bipartition side force the odd-time vanishing in step 2.1. Period uses positive return times, so the identity in [F1] does not enter ; steps 2.1–3.1 establish the positive-time gcd. The neighbor and path witnesses are used only for each fixed vertex as needed, so the argument uses no choice function or AC. There is no iff claim.
Source notes
LPW §1.3, printed pp. 7–8 (PDF pp. 23–24), defines period using positive return times, proves period invariance for irreducible chains in Lemma 1.6, and explains alternating support classes for a chain of period two; its Example 1.8 uses an even cycle. Section 1.4, printed p. 8 (PDF p. 24), defines simple random walk on an undirected graph by choosing a neighbor uniformly. These finite-chain passages do not prove the general locally finite bipartite-graph claim. The row definition, parity induction, backtrack, and connected-path transfer needed here are made explicit above.
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Sources
- Levin, Peres and Wilmer, Markov Chains and Mixing Times, second edition (standard reference, not scraped)