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Recurrence Transience and Hitting Times for Markov Chains
1 · Prerequisites
- Absolute and Conditional Convergence; Rearrangement; Products
- Binary Operations, Monoids, Groups and Subgroups
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Conditional Distributions and Regular Conditional Probability
- Conditional Expectation
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Discrete Time Martingales
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Equivalent Forms of Completeness
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Infinite Product Measures and Kolmogorov Extension
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Markov Kernels and Markov Chains
- Measurable Functions and Simple Approximation
- Measures and Their Basic Properties
- Metric Spaces
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Outer Measure and the Caratheodory Extension Theorem
- pi: the Equivalent Characterizations
- Polynomial Rings, the Division Algorithm and Roots
- Power Series and Real-Analytic Functions
- Probability Spaces Random Variables and Expectation
- Product Measures and the Fubini Tonelli Theorems
- Properties of the Integral and the Working FTC
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Roots, Rational Powers, and Classical Inequalities
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Sigma Algebras and Borel Sets
- Signed and Complex Measures Hahn and Jordan
- Simple Field Extensions and the Construction of the Complex Numbers
- Sine, Cosine, and the Definition of Pi
- Stopping Times and Optional Stopping
- Subspaces, Products, and Quotients
- Suprema and Infima
- The Derivative and the Mean Value Theorems
- The Exponential Function
- The Lebesgue Integral and the Convergence Theorems
- The Logarithm and General Powers
- The Lᵖ Spaces Holder Minkowski and Riesz Fischer
- The Radon Nikodym Theorem and Lebesgue Decomposition
- The Real Gamma and Beta Functions
- The Riemann Integral: Definition and Integrability
- The Topology of Euclidean Space
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Vector Spaces, Linear Subspaces, Span and Direct Sums
2 · Summary
This page develops countable-state, discrete-time recurrence and hitting-time theory from the transition-matrix and stopping-time conventions. It proves the matrix Chapman–Kolmogorov identities, communication-class results, renewal and Green-kernel criteria, class invariance and the irreducible dichotomy. It then treats harmonic hitting probabilities, finite-state Dirichlet problems, periods, and the recurrence classification of simple symmetric walks on .
The final sections develop nonnegative exit costs, superharmonic bounds, the Poisson equation for expected exit times, and Lyapunov estimates. AC is stated where canonical chain laws and probability interfaces require it; local matrix and drift calculations remain choice-free.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Transition matrices and n-step probabilities
Definition
Let be countable with sigma-algebra , and let be a probability kernel on it. For , set
where is the identity kernel, so . By Iterated transition kernels, each is a probability kernel. Since measures on countable discrete spaces are their singleton-weighted sums (Every measure on a countable discrete space is its weighted sum of Dirac measures), every row satisfies
No conditional-expectation version or choice function is used in this matrix definition.
Matrix Chapman–Kolmogorov equations
Statement
For and in countable ,
Facts & Assumptions
Given: A countable state space , a probability kernel on , , and .
Iterated kernels start with and satisfy . Iterated transition kernels
Kernel composition is defined by . Composition of probability kernels
Kernel composition is associative at each source point and measurable set. Kernel composition is well defined and associative
A measure on a countable discrete space is determined by its singleton weights and is their weighted sum. Every measure on a countable discrete space is its weighted sum of Dirac measures
An increasing sequence of nonnegative measurable functions passes to the limit under the integral. Monotone convergence for the integral
The transition probabilities are . Transition matrices and n-step probabilities
Proof
For all , . For , the composition formula in [F2] and in [F1] give . If the identity holds at , then [F1] and associativity [F3] give
Induction proves the kernel identity. [F1, F2, F3, given, induction]
Apply step 1.1 to the singleton . By [F2] and [F6], . The integrand is measurable and between zero and one because is a probability kernel, so the integral is defined.
If is finite, list it without repetition as ; if it is countably infinite, fix a bijection . Let in the finite case and in the infinite case, and set . These finite-support functions increase pointwise to and are constant once in the finite case. By [F4], the singleton weights of are ; [F5] therefore gives . Combining with step 2.1 proves the formula, with the nonnegative series interpreted by its finite partial sums.
If , the row leaves only the term ; if , leaves only . When , both sides are . Thus the zero-time endpoints, including the one-state and deterministic cases, agree. If , there are no and the assertion is vacuous. The proof uses kernel algebra and nonnegative sums only; no AC or conditional-probability version enters.
Accessibility, communication, and irreducibility
Definition
For the countable transition matrix of Transition matrices and n-step probabilities, define accessibility by
States communicate, written , when and . The chain is irreducible when every pair of states communicates. Because , every state is accessible from itself with a zero-step path.
Communication is an equivalence relation
Statement
For a countable transition matrix on , communication is an equivalence relation on , and its equivalence classes partition .
Facts & Assumptions
Given: A countable state space and its transition matrix .
Accessibility means exactly when for some . Accessibility, communication, and irreducibility
Communication is mutual accessibility: means and . Accessibility, communication, and irreducibility
The zero-step row satisfies , so each state is accessible from itself. Accessibility, communication, and irreducibility
Proof
By [F3], , hence and for every . The definition in [F2] is symmetric in , so communication is symmetric.
Suppose and . By [F1], choose with and . The nonnegative series in [F4] contains the term at , so . Thus . The argument permits either witness length to be zero.
If and , then gives by step 1.2, and gives by the same step. Therefore , proving transitivity of communication.
Define . Reflexivity makes each contain , so these classes cover . If , symmetry and transitivity give ; then every member of either class belongs to the other, so . Thus distinct classes are disjoint and the classes partition .
If , there are no states or classes and the assertion is vacuous. If has one state, step 1.1 gives its sole class. Absorbing or otherwise degenerate rows cause no exception: the proof uses only zero-step identity and positive accessibility witnesses. No global choice is made; for each fixed triple in step 1.2, the two existential witnesses are used locally.
Hitting, return, and visit times
Definition
Let be an adapted Stochastic processes and their finite-dimensional distributions with values in a countable set equipped with . For , define
The infimum of the empty set is . The visit count is the extended nonnegative integer
For a process started at , put and define recursively
Thus a later return time is assigned if the preceding one is infinite; the expression is never used. For every and ,
where the second union is empty when . Adaptedness makes these events belong to , so these are stopping times under Discrete stopping time.
Recurrent and transient states
Definition
For a specified Markov chain law with transition matrix and deterministic initial state , write for that law. The state is recurrent when
and transient when
Here is the strictly positive return time of Hitting, return, and visit times, so the initial visit at time zero does not count as a return. Since the displayed return probability lies in , these alternatives exhaust all states. The definition concerns the specified law and does not assert that laws for every state can be selected simultaneously.
Renewal decomposition at successive returns
Statement
Assume AC (The Axiom of Choice). Let be a Time-homogeneous Markov chain with transition kernel on an at most countable state space with transition matrix , and use for its law started at . Put Then and, for every ,
Let and let be the successive return times from Hitting, return, and visit times. For each and bounded measurable future-path functional , define with value when . The post-return path has law independently of on the event of a finite return, in the precise sense
An excursion word from is a finite sequence , , with and for . When , let the th completed excursion be ; set if , where . If is recurrent, all are finite almost surely and are iid. For a state that is not recurrent, the next excursion is asserted only after the preceding return is finite; no infinite sequence of completed excursions is asserted.
Facts & Assumptions
Given: AC, a countable-state Markov chain and a state .
Every family of nonempty sets has a choice function; AC is assumed for the conditional-expectation and Markov results used below. (The Axiom of Choice)
The return times are defined recursively, with , , and later returns set to after an infinite return. (Hitting, return, and visit times)
A map is a discrete stopping time when for every . (Discrete stopping time)
For a stopping time , . (Sigma-algebra at a stopping time)
For a chain with AC and bounded measurable , almost surely; the event version follows by taking an indicator. (Chapman-Kolmogorov equations)
If is a stopping time and is a bounded measurable future-path functional, then the conditional expectation of its shifted-path value is on , with the shifted value defined as zero at . (Discrete strong Markov property)
The state is recurrent exactly when . (Recurrent and transient states)
Under , the initial state is almost surely. (Initial distribution of a Markov chain)
A time-homogeneous Markov chain is adapted to its filtration. (Time-homogeneous Markov chain with transition kernel)
Every coordinate is a measurable random element, so finite-coordinate cylinder events are measurable. (Stochastic processes and their finite-dimensional distributions)
Proof
Since by [F4], . The conditional identity [F5] at , together with [F8] and the definition of [F4], gives .
Every recursively defined is a stopping time: is one, and if is one, then for , with the union empty when . For , is in because it is the difference of the stopping-time events and (with the case immediate). Adaptedness [F9] and the increasing filtration then put every displayed term in . This proves the induction using [F1, F2].
Let be the set of excursion words defined in the statement. It is countable because it is a countable union of finite products of the countable set . For any , let be the indicator that a path starting at has a finite first-return word in , and set it to zero if there is no positive return. Its event is a countable union of finite-coordinate cylinder events [F10], so is product-measurable and bounded; write .
Fix . The disjoint events , , partition , because any path ending at has a first positive visit by time . By [F5], on , since on that event. Summing these finitely many disjoint contributions and using step 1.1 gives the claimed renewal equation.
By step 1.2, is a stopping time. Apply [F6] to at . On , , and the shifted event is exactly that the next completed excursion word is in . Therefore where the left side is interpreted as zero when . The same strong Markov identity with arbitrary bounded gives the post-return formula in the statement.
Suppose is recurrent. Taking in step 2.2 gives by [F7]. Induction from yields for every ; since there are countably many , all returns are finite simultaneously almost surely.
For and arbitrary , the event belongs to : on each event it is determined by , so by [F3]. Applying the conditional identity in step 2.2 at and using step 3.1 gives Induction in factors this joint probability as , proving that the excursion words are iid with common first-excursion law .
If , there is no state and the theorem is vacuous. If has no positive return, then for every (a visit at positive time would be a return), every , and the convolution has both sides zero; for the identity is . At the endpoint , the formula is . In a one-state absorbing chain, , for , and , so the equation holds directly. More generally, in a deterministic cycle of length , and ; if the sum is empty, and if the sole possible term is , as required. For a transient state the conditional identities of steps 2.2 remain restricted to finite ; if a return fails, the definition sets later returns to infinity, and no further completed excursion is claimed. AC [A1] is used through [F5] and [F6]; the cylinder measurability and event decomposition use no additional choice. The equation and iid assertion are one-way claims, not biconditionals.
Equivalent criteria for recurrence and transience
Statement
Assume AC (The Axiom of Choice). Let be a time-homogeneous Markov chain on an at most countable state space , with transition matrix . Fix and use and for the specified law with almost surely. For the visit count , which includes the initial visit, the following are equivalent:
If is transient and , then for every integer ,
Facts & Assumptions
Given: AC, a countable-state Markov chain, and a fixed state .
AC is assumed for the specified chain law and the finite-dimensional and strong-Markov conditional-expectation interfaces used below. (The Axiom of Choice)
Under the fixed initial state, almost surely, and denote that specified law and expectation. (Initial distribution of a Markov chain)
counts the time-zero visit. (Hitting, return, and visit times)
, so a return must occur at a strictly positive time. (Hitting, return, and visit times)
The successive returns are and after a finite preceding return, with later returns set to after an infinite one. (Hitting, return, and visit times)
is recurrent exactly when , and is transient exactly when . (Recurrent and transient states)
The finite-dimensional law at the single time , with initial law and test , gives . (Finite-dimensional laws of a Markov chain)
At each finite return time , the post-return path has the law in the conditional sense: for bounded measurable future-path , a.s. (Renewal decomposition at successive returns)
Each coordinate is a measurable random element; hence its singleton event is measurable. (Stochastic processes and their finite-dimensional distributions)
If nonnegative measurable , then , allowing . (Monotone convergence for the integral)
For decreasing measurable events in the probability measure , because . (Continuity from above when one set has finite measure)
If , then . (For the sequence is null, and for the sequence diverges to )
If , then . (For , , and for the series diverges)
Integer powers use , including when . (For , , and for the series diverges)
Proof
For each , pathwise . Since [F1], the first visit is already counted, and at least visits are exactly further finite returns. In particular, both events are certain for since . Also .
The finite partial visit counts are nonnegative measurable by [F9] and increase pointwise to [F2]. Monotone convergence [F10] therefore gives, with extended values allowed, , where the last equality uses the finite-dimensional law [F7] under AC [A1]. The term is on each side by [F1] and [F6]; no initial visit is lost.
Define the bounded future-path functional . Its event is a countable union of coordinate-cylinder events, hence measurable by [F9], and by the definition of [F3]. On , ; on it is zero. Applying the AC-based strong-Markov identity [F8] and taking expectations gives . Starting from , induction yields . By step 1.1, for every .
The events decrease to . Continuity from above [F11] and step 2.1 give . If is recurrent, [F5] gives , so this limit is . If is transient, [F5] gives , and [F12] makes the limit . These two cases exhaust all states, so is recurrent if and only if .
For , let . These are nonnegative measurable variables, increase pointwise to , and [F10] together with step 2.1 gives . If is recurrent then [F5] gives and this sum is . If is transient then [F5] gives and [F13] gives . In view of step 1.2, the Green series diverges exactly in the recurrent case. This proves both directions of the recurrence/Green-series equivalence without subtracting extended values.
In the transient case, for every the nested tail events satisfy by step 2.1 and finite subtraction of probabilities in . Since by step 3.1, these masses account for all outcomes; their sum is by [F13]. When , the convention [F14] gives and for , as expected when no positive return occurs. The mean formula is the transient case of step 3.2.
If , there is no and the theorem is vacuous. For a one-state absorbing chain, , almost surely, and for every , agreeing with both recurrence criteria. If a deterministic chain started at leaves and never returns, then , almost surely, and for , agreeing with the transient formulas. If instead a deterministic cycle returns after a fixed positive period , then and for all , so both the infinite-visit probability and Green series are infinite as asserted. The Green term and tail were treated explicitly in steps 1.1 and 1.2–3.2. AC [A1] is used for the specified chain law and the conditional strong-Markov identity [F8]; the return-series arithmetic itself uses no choice. Both stated equivalences have been proved in both directions in steps 3.1 and 3.2.
Green kernel of a transient chain
Definition
For any countable transition matrix , define its extended nonnegative Green kernel by
This matrix series is defined without Choice. Under the explicitly assumed Axiom of Choice The Axiom of Choice, for a specified chain law with initial state , the multistep Markov identity gives for each (Chapman-Kolmogorov equations). Applying monotone convergence to the partial sums of then gives
No finiteness is asserted: may be , including when a chain starts in a transient state and can enter a recurrent class. The expectation identity uses Hitting, return, and visit times and Monotone convergence for the integral; the matrix definition remains valid for recurrent states as well.
Green-kernel resolvent identity
Statement
Let be at most countable, let be a transition matrix on , and let . Define the extended nonnegative matrix products by the support-restricted sums
Zero-coefficient terms are omitted, so neither product forms the undefined . Then, for every ,
with all sums and equalities in the nonnegative extended reals.
Facts & Assumptions
Given: An at most countable state space and a transition matrix on .
The Green kernel is . Green kernel of a transient chain
For , the nonnegative kernel action is . Nonnegative kernel action and finite drift
A nonnegative double series has the same value in either summation order: , including when the common value is . Tonelli's theorem for double series of nonnegative extended real numbers
In the library's extended-real arithmetic, every product with one factor and the other is undefined. The extended real line , its order, and the arithmetic that is left undefined
A countable set is finite or is in bijection with . Finite, countably infinite, countable, uncountable
The zero-step transition probability is . Transition matrices and n-step probabilities
A nonnegative extended series is the supremum of its finite partial sums. Series in the nonnegative extended real line
Proof
If is a finite positive real and is nonnegative, then . For partial sums , if , continuity of multiplication by gives ; if , the are unbounded and so are . By [F5], every product is defined because .
Fix . For each with , [F1, F2] and step 1.1 give . Terms with are omitted in ; inserting corresponding zero terms in the nonnegative double series is valid because . Apply [F4] to that double series. If is finite, use a finite listing and pad with zeros; if countably infinite, use a bijection with from [F6]. Then [F3] with yields
For each with , [F1] and step 1.1 give . Terms with are omitted in ; inserting their zero finite products in the double series introduces no undefined extended-real product. Tonelli [F4], now summing first over , and [F3] with and second time index give
By [F1, F8], separating the term in the nonnegative series gives . This is a split of nonnegative partial sums, not a subtraction. Using [F7] and steps 2.1 and 2.2 proves both identities. If , there are no and the claim is vacuous. For a one-state absorbing chain, and both support-restricted products equal , so is well defined. Zero transition coefficients are always omitted; positive coefficients may multiply and produce . The argument includes deterministic rows and all zero-time endpoints. It uses no AC: the one enumeration of this fixed countable is part of [F6], and [F4] is proved using finite choice. The lemma states no biconditional.
Recurrence and transience are class properties
Statement
Assume AC (The Axiom of Choice). Let be at most countable with sigma-algebra , and let be a probability kernel with transition matrix . For each fixed , let be the canonical path-space law with initial measure and transition kernel . Write and . If and communicate, then More strongly, if is recurrent and , then The communicating class of a recurrent state is closed: if and , then .
Facts & Assumptions
Given: AC, an at most countable state space with its full power-set sigma-algebra, a probability kernel , its transition matrix , and the canonical law for each fixed deterministic start.
Every family of nonempty sets has a choice function. AC is used for the canonical chain laws and the conditional Markov suppliers cited below. (The Axiom of Choice)
An at most countable set is finite or countably infinite. (Finite, countably infinite, countable, uncountable)
A probability kernel is a measure in its target variable and has total mass one. (Measure kernel and probability kernel)
The transition entries are , and matrix powers are defined from the iterated kernels. (Transition matrices and n-step probabilities)
For each , the Dirac set function is a probability measure. (A Dirac set function is a probability measure)
Under AC, the canonical path space has the chain law with specified initial measure and transition kernel. (Canonical Markov chain on path space)
With initial state fixed at , ; in particular almost surely under . (Initial distribution of a Markov chain)
Accessibility means exactly when for some ; communication is mutual accessibility. (Accessibility, communication, and irreducibility)
For , . (Matrix Chapman–Kolmogorov equations)
The finite-dimensional law of the coordinate chain gives the probability of every finite cylinder as the product of its successive transition probabilities when the initial state is fixed. (Finite-dimensional laws of a Markov chain)
and are stopping times; the time-zero and positive return conventions are distinct. (Hitting, return, and visit times)
A state is recurrent exactly when ; transience means the probability is less than one, so the two cases exhaust all states. (Recurrent and transient states)
If is recurrent, all its successive returns are finite almost surely and the completed return excursions from are iid. (Renewal decomposition at successive returns)
At a stopping time, the conditional law of a bounded measurable future path functional is the law started from the state at that time on the event the stopping time is finite. (Discrete strong Markov property)
Communication is an equivalence relation, and its equivalence classes partition . (Communication is an equivalence relation)
If , then . (For the sequence is null, and for the sequence diverges to )
Proof
Fix distinct with . By [F7], the set of with is nonempty; choose its least element. It is positive because by [F3]. Repeatedly decompose a positive -step entry by [F8]. At each decomposition, some summand is positive, so this gives a finite route with This is a witness for this fixed pair only; it makes no simultaneous choice of routes. Minimality of implies and for , since either repeated endpoint would leave a shorter positive route from to . The finite-dimensional law [F9], with initial state [F6], gives Call this cylinder event . In particular, on the chain reaches before any positive return to .
If , recurrence of is the same assertion as recurrence of ; also under , so both hitting probabilities in the stronger claim equal one. This separates time-zero hitting from the strictly positive return used in [F11].
Suppose is recurrent and . By [F12], the return excursions are iid and finite almost surely. Let be the set of completed excursion words whose first transitions follow the route in step 1.1. Since contains no return to before time , the event agrees with except on the null event that the first return to is infinite. Hence , and the same holds for each excursion by identical distribution. For every , the probability that none of the first excursions begins with the route is . If , none of them can begin with it; therefore Since , [F15] makes the right side tend to zero. Thus .
Still suppose is recurrent and . Let be the indicator of the measurable future-path event that no coordinate equals . Put . Apply [F13] at the deterministic stopping time from step 1.1. Since on , the conditional future probability of avoiding is , so On this event there is no positive-time return to : the route has no intermediate , its endpoint is not , and the future avoids . If this contradicts [F11]. Hence and .
Under , let . Step 2.2 gives almost surely, and because . Apply [F13] at to the bounded future-path indicator . By step 2.1, its probability from is one. Thus after the chain first reaches it reaches again almost surely. This is a positive-time return from the initial state , so is recurrent by [F11].
Assume is recurrent, as required for the closure claim. Let and suppose . By [F14], , so some has by [F7]. The one-step transition and [F8] give so . If , steps 2.1 and 2.2 give ; if , membership is immediate. Thus , proving the class is closed.
Suppose . If is recurrent, then either as in step 1.2 or and step 3.1 shows is recurrent. If is recurrent, apply the implication of steps 2.1–3.1 to the ordered pair to get that is recurrent. This proves both directions of the equivalence. By [F11], a state that is not recurrent is transient, so the classification is shared.
If , there is no starting state and the assertions are vacuous. If has one state, its only transition row has probability one on itself; the state is recurrent and its class is closed. Zero transition weights cannot appear in the chosen route because every factor is positive; the Chapman–Kolmogorov sums otherwise include all states. For a deterministic transition map, recurrence of means its orbit returns to after some positive number of steps, so the orbit is a finite cycle; every state accessible from lies on that cycle and has the stated hitting and recurrence properties. The endpoint gives accessibility at time zero but recurrence still uses at positive time [F10, F11]; distinct communicating states use a route of length at least one. AC [A1] supplies the canonical fixed-start laws and is assumed by the renewal and strong-Markov results. The finite-route witness is selected only for each fixed pair, with no global route selection. The two recurrence implications were proved in step 4.1, so both iff cases are covered.
Source notes
Durrett, Probability: Theory and Examples, 5th ed., §5.3, Theorem 5.3.2 and its complete proof, printed p. 282/PDF p. 289 (official PDF parser lines 19113–19149). Durrett defines and proves that recurrence is contagious: recurrent and imply that is recurrent and . The proof first extracts a shortest positive route and shows by ruling out a positive-probability route followed by avoidance of ; it then uses Theorem 5.3.1's Green-series criterion to establish recurrence of . Here that last conclusion follows instead from the proved iid excursion law and strong Markov at . No diagonal-series comparison is used. The exact countable-state theorem is the Durrett source for the claim; its argument is not treated as a substitute for the complete local proof.
Levin–Peres–Wilmer, Markov Chains and Mixing Times, 2nd ed., §21.1, Proposition 21.3 and its complete proof, printed pp. 291–292/PDF pp. 307–308 (official PDF parser lines 22015–22090). The source assumes irreducibility and proves the equivalent all-state recurrence and hitting statements. It is relevant after restriction to a closed communicating class but is not used in this local proof. Section 1.7, printed pp. 15–17/PDF pp. 30–32, supplies finite-state communicating-class terminology only.
Irreducible recurrence/transience dichotomy
Statement
Assume AC. Let the countable-state chain, transition matrix, fixed-start canonical laws, and positive-time recurrence convention be as in Recurrence and transience are class properties. Irreducibility means that every pair of states communicates (Accessibility, communication, and irreducibility). If , the universal conclusions below are vacuous. Otherwise, if the chain is irreducible, then either every state is recurrent or every state is transient.
Facts & Assumptions
Given: AC and a chain in the countable-state setup of the class-property theorem.
AC supplies the fixed-start canonical laws and is an explicit hypothesis of the class-property theorem used here. (The Axiom of Choice)
Irreducibility means for every pair . (Accessibility, communication, and irreducibility)
Communicating states have the same recurrence status. In particular, recurrence of one state transfers to every state that communicates with it. (Recurrence and transience are class properties)
A state is recurrent when its positive-time return probability is one and transient when that probability is less than one; these alternatives exhaust all states because the probability lies in . (Recurrent and transient states)
Every probability-kernel row has total mass one. On a one-state space, this forces the sole transition probability to equal one. (Measure kernel and probability kernel)
Proof
If , there are no states to classify. Both universal conclusions in the disjunction hold vacuously.
Now suppose and fix one state . For every , irreducibility [F1] gives . This fixes one witness state only; no family of choices is made.
If is recurrent, [F2] and step 1.2 imply that every is recurrent. Hence the first alternative holds.
If is not recurrent, consider any . If were recurrent, [F2] and step 1.2 would imply that is recurrent, a contradiction. Thus no state is recurrent. By [F3], every state is transient, so the second alternative holds.
By [F3], the fixed state is either recurrent or transient. Step 2.1 handles the recurrent case and step 2.2 handles the transient case. Therefore one of the two asserted universal alternatives always holds.
If has one state , [F4] gives , so its positive-time return probability is one. If has more than one state, an absorbing row at any state would make the chain reducible; zero one-step weights are allowed, since irreducibility requires communication by some positive-probability finite path, not a positive one-step transition. The zero-step accessibility alone does not establish recurrence, which requires a positive-time return [F3]. For a deterministic transition map on a nonempty irreducible state space with more than one state, fix and choose . The unique forward orbit from reaches and then returns to by irreducibility. It therefore contains a finite cycle through ; every state is reachable from , so every state lies on this cycle and returns to itself. Steps 2.1 and 2.2 prove the forward and reverse uses of the class-property equivalence. AC [A1] is inherited by the canonical laws and class-property theorem; fixing one state in step 1.2 uses no choice principle.
Source notes
Durrett, Probability: Theory and Examples, 5th ed., §5.3, Theorem 5.3.2 and its complete proof, printed p. 282/PDF p. 289 (official PDF parser lines 19113–19149), proves the stronger countable-chain statement that recurrence is contagious along accessibility and that the reverse hitting probability is one. Example 5.3.6 explicitly says that an infinite irreducible chain is either wholly recurrent or wholly transient, printed p. 284/PDF p. 291 (official parser lines 19241–19243). The example alone has an infinite-state hypothesis; this item's finite and empty cases are handled locally. The proof here uses the pair's completed class-property theorem and the definition that recurrence and transience exhaust the return-probability alternatives.
Hitting probability as minimal harmonic extension
Statement
Assume AC (The Axiom of Choice). Let be a Markov chain with transition kernel on an at most countable state space , transition matrix , and let . Define . Then where is the support-restricted nonnegative kernel action. Moreover, for every finite-valued satisfying on and on , one has for every .
Facts & Assumptions
Given: AC, a countable-state Markov chain, , and for the minimality claim a finite-valued nonnegative with on and on .
The Axiom of Choice states that every family of nonempty sets has a choice function; it is assumed by the canonical-law and conditional-expectation/Markov suppliers used below. (The Axiom of Choice)
, so at a start in . (Hitting, return, and visit times)
The infimum of the empty set is . (Hitting, return, and visit times)
For nonnegative , , omitting zero transition weights. (Nonnegative kernel action and finite drift)
A measure on a countable discrete space is the sum of its singleton weights; for those weights are . (Every measure on a countable discrete space is its weighted sum of Dirac measures)
For bounded product-measurable , is measurable and almost surely. (Markov property for bounded future path functionals)
For bounded measurable , almost surely. (Bounded-function form of the Markov property)
Under , one has almost surely. (Initial distribution of a Markov chain)
For nonnegative measurable , is characterized by its event integrals, and increasing nonnegative limits pass through conditional expectation almost surely. (Conditional monotone convergence)
For bounded real , . (Basic algebra and order properties of conditional expectation)
Fatou's lemma gives for nonnegative measurable . (Fatou's lemma)
Increasing sequences of nonnegative measurable functions pass to the limit under the nonnegative integral. (Monotone convergence for the integral)
A nonnegative simple measurable function has finite range. (Nonnegative simple measurable functions)
The nonnegative Lebesgue integral is defined as the supremum of the simple integrals of nonnegative simple minorants. (The nonnegative Lebesgue integral)
For on disjoint measurable sets, its simple integral is . (The integral of a nonnegative simple function)
For every nonnegative simple measurable , its nonnegative Lebesgue integral equals its simple integral. (The nonnegative integral agrees with the simple integral on simple functions)
A nonnegative extended series is the supremum of its increasing finite partial sums. (Series in the nonnegative extended real line)
Proof
If is finite or countably infinite, fix an increasing finite exhaustion (using a fixed enumeration when is infinite), and for put . Each is bounded and simple by [F12]; the nonnegative integral [F13], its simple-function agreement [F15], the simple integral formula [F14], the atomic weights [F4] and [F2] give . As , [F11] passes the integrals to , while the finite sums increase to the support-restricted extended row sum by [F16] and [F3]; thus , with zero weights omitted and no formed.
If , there is no state or initial law to check; if , then by [F1, F17], so and follows from ; if , every start has and , while every admissible is also ; in general, [F1, F7] give whenever .
Define , a bounded product-measurable path functional. By [F5], is measurable and ; for , hitting is equivalent to the shifted path hitting it, so [F9] gives . The bounded one-step identity [F6], [F7], and expectation preservation [F9] identify this as ; step 1.1 then gives .
For any finite-valued nonnegative and each , use the finite-support truncations from step 1.1. The bounded one-step identity [F6] and step 1.1 give ; since , conditional monotone convergence [F8] and the row-sum limit in step 1.1 yield almost surely, with its event-integral characterization available even when the conditional value is infinite.
Fix , put , , and by [F1]. If , then on one has and ; [F8] and step 2.2 give . On , , and on , and . Since by [F7], induction from proves and integrability for every finite .
On , for every , while on all ; hence . Fatou [F10] and step 3.1 give for , and step 1.2 covers , , and . A one-state absorbing chain is included by those same two set cases, and the finite-row argument in step 1.1 covers deterministic transitions. AC [A1] is used for the canonical laws and the conditional-expectation/Markov suppliers; the row exhaustion uses the supplied countability witness, with no extra choice. The result asserts minimality and no biconditional.
Geometric tail for hitting in a finite irreducible chain
Statement
Assume AC. Let be finite, let be an irreducible transition matrix on , and let be nonempty. There exist an integer and such that, for every and ,
In particular, for every . Moreover, in any countable-state chain with transition matrix , if is a finite nonempty subset satisfying for each and the restricted matrix on is irreducible, then every state of is recurrent for .
Facts & Assumptions
Given: AC. The geometric-tail clause assumes a finite state space , an irreducible transition matrix , and a nonempty target . The recurrence clause assumes a countable state space , a transition matrix , and a finite nonempty that is closed under and irreducible for the restricted matrix.
Irreducibility means every pair of states communicates, with accessibility witnessed by some finite matrix power. Accessibility, communication, and irreducibility
The transition probabilities are , where is the one-step kernel. Transition matrices and n-step probabilities
The hitting time is and is a stopping time; in particular . Hitting, return, and visit times
Under the deterministic initial state , the chain law and expectation are denoted and . Initial distribution of a Markov chain
For bounded measurable future path functionals , with . Markov property for bounded future path functionals
Finite-dimensional chain laws give . Finite-dimensional laws of a Markov chain
For a nonnegative random variable, expectation is the integral of its strict tail probabilities. Layer-cake formulas for random variables
A state is recurrent when . Recurrent and transient states
Full AC supplies a choice function for a family of nonempty sets; here it is assumed for the canonical chain-law and conditional-Markov interfaces in [F5] and [F6]. The Axiom of Choice
Proof
Fix one . For , irreducibility gives a nonempty set ; let be its least element. Set for . By [F2] and [F6], for every : it is on , and off the event has positive probability. Since is finite, is finite and for every . Thus lies in and uniformly. The witness lengths are least natural numbers, so this finite construction makes no choice-function assumption.
Define the bounded path functional and . Step 1.1 gives for every . For let by [F3]. The event is intersected with avoidance of during the next steps. Applying [F5] at time and integrating over yields . This unconditional recursion also holds when a survival event has probability zero.
Since , induction in step 2.1 gives for every . Since is integer-valued (with allowed), its strict tail is constant on each interval ; integrating that tail in [F7] gives . Writing with and using monotonicity of the tail, This bound is uniform in .
The same estimate gives the scaffold's finite-class return consequence. For this clause, let be countable and let be finite and nonempty, satisfy for each , and have an irreducible restricted matrix. For each , closure and the finite-dimensional iterated law [F6] imply for every and identify the joint law of with that of the restricted matrix on . In particular, each event has the same probability under the ambient and restricted chains; summing these integer tails by [F7] shows their hitting-time expectations agree. Fix and put by applying the argument of steps 1.1–3.1 to this finite restricted chain. For every , the bounded future-path Markov identity at time , applied to avoidance of in the next coordinates, gives Summing this identity over and using the same integer-valued tail identity from [F7] as in step 3.1 gives . Hence , so [F8] makes recurrent. Since was arbitrary, every state of is recurrent.
The nonempty-target hypothesis is necessary: for , and the finite-mean conclusion fails. If or the starting state lies in , then and the tail bound holds immediately; for a one-state chain these are the only target cases. Deterministic and other degenerate rows are covered by the same positive accessibility witnesses and the uniform block estimate. At the asserted bound is just . AC is used only through [F5] and [F6]; all path-length witnesses above are least natural numbers. The theorem is not an iff statement.
Bounded Dirichlet problem for hitting probabilities
Statement
Assume AC (The Axiom of Choice). Let be a Markov chain with transition kernel on an at most countable state space and transition matrix . If , the assertion is vacuous. For , suppose for every . For bounded real boundary data , define the payoff before any random-time evaluation by Then is the unique bounded satisfying where for bounded real , is absolutely convergent. In particular, the almost-sure hitting hypothesis holds when is finite, is irreducible, and is nonempty. For on , .
Facts & Assumptions
Given: AC; a Markov chain on an at most countable discrete state space with transition matrix ; a set ; bounded real data on ; and for every deterministic start .
AC is the axiom that every family of nonempty sets has a choice function; the canonical chain-law and conditional-expectation Markov interfaces below assume it. (The Axiom of Choice)
The transition probabilities satisfy and every kernel row is a probability measure; in particular its singleton weights sum to one. (Transition matrices and n-step probabilities)
, with ; hence is a stopping time and is defined for finite . (Hitting, return, and visit times)
Under the deterministic start, , is its expectation, and almost surely. (Initial distribution of a Markov chain)
For bounded measurable , (Bounded-function form of the Markov property)
For bounded product-measurable path functionals , is measurable and (Markov property for bounded future path functionals)
On bounded real functions, ; the series is absolutely convergent since . (Discrete generator of a countable-state transition matrix)
A nonnegative function with finite range is simple; its simple integral is the finite sum of its values times the measures of its disjoint level sets, and this equals its nonnegative Lebesgue integral. (Nonnegative simple measurable functions, The integral of a nonnegative simple function, The nonnegative integral agrees with the simple integral on simple functions)
For an integrable real , its integral is . (Integrable real and complex functions, and their integrals)
Dominated convergence passes limits through integrals when the functions converge almost everywhere and are bounded by one integrable majorant. (Dominated convergence)
Conditional expectation preserves order and constants and satisfies for integrable real . (Basic algebra and order properties of conditional expectation)
If is finite, is irreducible, and is nonempty, there are and such that for every and . (Geometric tail for hitting in a finite irreducible chain)
Source scope
LPW Proposition 9.1 and its proof [S1] give context for the boundary-payoff construction and the first-step decomposition. Its uniqueness argument uses a global maximum, and its displayed assumptions do not supply the almost-sure boundary-hit and bounded-data hypotheses used here; that argument is not invoked for the countable bounded result. Roch Theorem 24.4 [S2] proves the first-step equations for bounded nonnegative exit data on a proper domain. The bounded real-data equations and the uniqueness statement below are derived locally under the stated almost-sure hitting assumption.
Proof
Proof technique: establish the bounded row-integral identity by finite support truncations, derive the boundary and harmonic equations from bounded Markov identities, and identify every bounded solution by a stopped martingale and dominated convergence.
Fix and a bounded real , with . Take an increasing sequence of finite sets (eventually if is finite) and put . The positive and negative parts of are finite-range nonnegative simple functions. By [F1], [F7] and [F8], The constant is integrable for the probability measure , so [F9] gives . Also by [F1], so the finite sums converge to the absolutely convergent row sum from [F6]. Therefore This identity holds for every bounded real and each row; no positivity of the individual entries beyond being transition weights is required.
Choose with on , extend by zero off , and define to be when the first-hit time of is finite, and zero otherwise. Each event that the first hit is at time is cylinder-measurable; is the pointwise limit of its finite sums over these disjoint events, so it is product-measurable and . By [F5], is measurable; [F10] gives . The payoff in the Statement equals pathwise, including its zero value on nonhit paths, so . If , [F2] and [F3] give and . If , deleting the first coordinate does not change , including when the path never hits . Thus [F5] at time and [F10] give Apply [F4] at time to the bounded function , use [F3] and [F10] to take expectations, and then use step 1.1 to obtain This proves existence and both equations.
Let be any bounded solution of the stated boundary and harmonic equations, fix , set , and define . By [F2] this is adapted, and it is bounded by . On , ; on , and . The one-step identity [F4], the row identity in step 1.1, and on imply Consequently is a bounded martingale and [F3], [F10] give for every . The hypothesis makes -almost surely, so eventually almost surely. Since is an integrable majorant, [F9] yields As was arbitrary, every bounded solution equals ; this proves uniqueness.
If is finite, is irreducible and , [F11] gives , so the almost-sure hitting hypothesis holds for every start. The preceding steps give the finite irreducible instance. When on , the pathwise payoff is , hence its expectation is the hitting probability; under the theorem's hypothesis it equals .
If , there is no state or deterministic-start law and all assertions are vacuous. If and , then everywhere, contradicting the hypothesis; thus every nonvacuous instance has . If , then , the boundary equation determines and every solution directly. For a one-state chain these are the only admissible cases. If , then and the uniqueness proof still applies. Deterministic rows are covered by the row identity and the same martingale calculation; a finite irreducible deterministic chain reaches every nonempty by the finite-tail argument. The endpoint is handled in step 2.1, while a first hit at time is included in the shifted-path and stopped-process identities in steps 2.1 and 2.2. AC [A1] is used through the canonical chain laws and conditional-expectation Markov identities [F4], [F5] and [F10]; choosing one enumeration of a countable adds no family-wise choice. The equations and uniqueness claim are not an iff statement.
Period of a state
Definition
For , let
If , set . If , define to be the greatest positive integer dividing every element of (the gcd convention of Common divisor, and the greatest common divisor , with the convention ). This greatest divisor exists: fix one ; every common positive divisor of is a divisor of , so the set of such divisors is a nonempty finite subset of the positive divisors of , and therefore has a greatest element. The set being maximized is intrinsic to , so the result is independent of the auxiliary . Only positive return times enter; does not force .
Period is constant on communicating classes
Statement
If and communicate, then , including and the convention when no positive return exists.
Facts & Assumptions
Given: A countable transition matrix and communicating states .
Communication means and , where accessibility is witnessed by some with . Accessibility, communication, and irreducibility
; if , and otherwise is the greatest positive integer dividing every element of . Period of a state
Proof
If , the conclusion is the identity , whether or not is empty. Suppose . By [F1], choose route lengths with and . By [F4], neither length is zero, so . Twice applying [F3] and retaining the route terms gives and . Thus both return-time sets are nonempty and both periods are positive.
Fix any . By [F3], the route from to , a -step return at , and the route from to give . Step 1.1 also shows . Hence the positive integer divides both and , so it divides their difference . As this holds for every , is a common positive divisor of and therefore by [F2].
Interchanging and in step 2.1 shows that every is divisible by ; hence is a common positive divisor of and . Together with step 2.1 this proves equality for distinct communicating states. The case was settled in step 1.1.
If , there are no communicating states and the assertion is vacuous. If and there is no positive return, both sides equal the stipulated zero; if communicate, step 1.1 proves positive returns exist, so neither period is zero. One-state, deterministic, and absorbing cases are covered by the same alternatives. The accessibility witnesses are positive for distinct states because [F4] makes a zero-step transition possible only from a state to itself. The proof chooses routes only for this fixed pair, so it uses no choice function. This one-way equality statement is not an iff.
Aperiodic irreducible chain
Definition
Let be an irreducible transition matrix on a nonempty countable state space . The periods are independent of by Period is constant on communicating classes, and the verification below shows their common value is positive. Define the period of the chain by for any . The chain is aperiodic when .
Facts & Assumptions
Given: A nonempty countable state space and an irreducible transition matrix on .
Every transition-matrix power has a stochastic row: . (Transition matrices and n-step probabilities)
The zero-step matrix is . (Transition matrices and n-step probabilities)
Irreducibility means every pair of states communicates. (Accessibility, communication, and irreducibility)
Accessibility is witnessed by a finite with . (Accessibility, communication, and irreducibility)
The positive return set is ; if it is nonempty, is its greatest common positive divisor, while if . (Period of a state)
For , . (Matrix Chapman–Kolmogorov equations)
Communicating states have equal periods, including the convention that a state with no positive return has period zero. (Period is constant on communicating classes)
Verification
For each , is nonempty. If , [F1] gives , so . If has at least two states, fix an arbitrary and take ; by [F3]–[F4], there are with and . Since , [F2] forces , and [F6] gives . Thus is a positive integer by [F5] in either case.
For any , irreducibility [F3] makes them communicate, so [F7] gives . Step 1.1 shows this common value is positive. It is therefore independent of the chosen state and defines ; declaring aperiodicity by the condition is well-defined.
The empty state space is excluded in the definition because no state period could be chosen as a common value. For a one-state chain, step 1.1 gives period one and hence aperiodicity. On a deterministic cycle of length , label the states and let the transition from go to with probability one. Iteration gives when divides and zero otherwise, so positive return times are precisely the positive multiples of and the period is ; a one-state absorbing chain is the case . The return set begins at , so does not make every chain aperiodic. The proof uses only fixed-pair routes and finite row sums, with no choice function or AC. This is a definition, not an iff theorem.
Simple symmetric walk on the integer lattice
Definition
For an integer , the simple symmetric nearest-neighbor transition matrix on is
with every other entry zero. Here is the th standard basis vector. The neighbors are distinct when , so each row sums to ; this is a transition matrix in the sense of Transition matrices and n-step probabilities. The definition uses no Choice.
One-dimensional simple symmetric walk is recurrent
Statement
Assume AC. Identify with and define, for , For each fixed , use the canonical chain law with initial measure and kernel . This is the simple symmetric nearest-neighbor walk in dimension one (Simple symmetric walk on the integer lattice). With , every state is recurrent:
Facts & Assumptions
Given: AC, the state space with its full power-set sigma-algebra, the one-dimensional simple symmetric walk, and a fixed start .
AC is assumed by the canonical path-law and finite-dimensional-law suppliers used here. (The Axiom of Choice)
In dimension one, the simple symmetric transition row has mass at each of the two distinct neighbors , and zero elsewhere. (Simple symmetric walk on the integer lattice)
For each point , is a probability measure. (A Dirac set function is a probability measure)
A finite nonnegative weighted sum of measures is a measure. (Nonnegative scalar multiples and countable weighted sums of measures are measures)
A probability kernel is a measure in its target variable for each source point, has total mass one, and is measurable in the source point for each measurable target set. (Measure kernel and probability kernel)
A function is measurable when the preimage of each measurable target set is measurable in the source space. (A measurable function between measurable spaces)
Under AC, the path space carries the canonical law for a specified probability initial measure and probability kernel. (Canonical Markov chain on path space)
With initial measure , the fixed-start notation is and almost surely. (Initial distribution of a Markov chain)
Under the finite-dimensional law, the probability of a finite cylinder is the iterated product of its initial and transition probabilities. (Finite-dimensional laws of a Markov chain)
The matrix entries are and , with . (Transition matrices and n-step probabilities)
is the number of -element subsets of an -element set. (The set of -element subsets and the binomial coefficient )
For a fixed state, recurrence is equivalent to divergence of its return Green series: is recurrent iff . (Equivalent criteria for recurrence and transience)
Recurrence means that the positive-time return probability is one. (Recurrent and transient states)
is the strictly positive return time. (Hitting, return, and visit times)
A set in bijection with is countably infinite and hence at most countable. (Finite, countably infinite, countable, uncountable)
Proof
Define by , , and for . Every integer occurs exactly once, so this is a bijection and is countably infinite, hence at most countable as required by the chain-law and recurrence suppliers.
For each fixed , the two Dirac measures in the displayed definition of are probability measures [F2]; their weighted sum is a measure by [F3], and its total mass is . For each fixed , the map is measurable because every subset of the discrete source is measurable [F5]. Thus [F4] makes a probability kernel. Its singleton entries agree with [F1], so this is exactly the d=1 simple symmetric walk kernel.
Under AC [A1], [F6] supplies the canonical law with initial measure for each fixed ; [F7] names it , and [F8] gives the probabilities of its finite path cylinders. The transition matrix of this chain is the matrix in [F9].
Fix and . A sign word determines the path for . Each such cylinder has probability by [F1], [F7], and [F8]. Distinct sign words give disjoint cylinders, and their endpoint equals exactly when the word has equally many and entries. By [F10] there are such words. Consequently For , this says , as required by [F9].
A sum of an odd number of increments is odd and cannot be zero. Thus for every .
Put . By step 1.4 and [F14], as . Hence there is such that for ,
For each integer , there are integers in , and for each one . Therefore Infinitely many such disjoint blocks show ; [step 2.1] then gives . The odd-time terms are zero by step 1.5, so the full Green series diverges. The initial term is and is included.
By [F11], divergence of the Green series implies that this fixed state is recurrent; by [F12] and [F13], this means exactly . Since was arbitrary, the conclusion holds for every state of . This uses only the forward implication of [F11], and no converse to the corollary is asserted.
The state space is fixed as , which contains and infinitely many integers, so the empty-space and one-state cases are inapplicable. Every row has two distinct positive transitions, so the walk is neither absorbing nor deterministic. Zero return weights occur at every odd time by step 1.5; the time-zero Green term is but is not a positive-time return [F12, F13]. AC [A1] is used exactly for the canonical path law and the stated finite-dimensional and recurrence suppliers. The enumeration of , the finite path count, and the square-block divergence require no choice. The only iff input is [F11]; the proof uses its divergence-to-recurrence direction, so the reverse direction is not part of the claim.
Source notes
Durrett, Probability: Theory and Examples, 5th ed., §5.4, Theorem 5.4.3 and complete proof (printed pp. 288–289/PDF pp. 295–296, official parser lines 19430–19460) gives the general return-series criterion for random walks. The d=1 part of Theorem 5.4.4 (printed p. 289/PDF p. 296, lines 19461–19469) uses odd-time parity and the central-order return probability to conclude recurrence. Its asymptotic is cited there from Theorem 3.1.3; here the published central-binomial asymptotic is used and the divergence is proved by square blocks. Durrett's source proof supports the result but does not replace the local kernel construction, finite-word calculation, or statewise Green-series argument above.
Two-dimensional simple symmetric walk is recurrent
Statement
Assume the Axiom of Choice (The Axiom of Choice). Put with its full power-set sigma-algebra. For and , define where and . For each fixed , let be the canonical path-space law with initial measure and kernel , and let be its transition matrix. Then every state is recurrent: where .
Facts & Assumptions
Given: AC, , its full power-set sigma-algebra, and the four-neighbor kernel in the Statement.
AC is the axiom that every family of nonempty sets has a choice function; the canonical-chain construction and recurrence criterion below explicitly assume it. (The Axiom of Choice)
is the quotient and its quotient map is onto. (The integers as equivalence classes of pairs of naturals)
; a nonempty set is at most countable when a surjection from onto it exists; bijections invert and surjections compose. (, Equinumerous sets, and , A nonempty set is at most countable iff it is a surjective image of , Injection, surjection, bijection, Finite, countably infinite, countable, uncountable)
The product of two at-most-countable sets is at most countable. (A product of two at most countable sets is at most countable)
A Dirac measure is a probability measure, and a finite nonnegative weighted sum of measures is a measure. (The Dirac set function at a point, A Dirac set function is a probability measure, Nonnegative scalar multiples and countable weighted sums of measures are measures)
A probability kernel is pointwise a measure of total mass one and is measurable in its source variable for each measurable target set. The measurability test is preimages of Borel sets. (Measure kernel and probability kernel, A measurable function between measurable spaces)
For , the simple symmetric lattice matrix has mass at each distinct neighbor and zero elsewhere. (Simple symmetric walk on the integer lattice)
Under AC, the canonical path space carries a Markov chain with specified initial probability measure and probability kernel; for initial , the notation is . (Canonical Markov chain on path space, Initial distribution of a Markov chain)
The transition entries and their iterates are and , with the identity at . (Transition matrices and n-step probabilities)
For a countable transition matrix, . (Matrix Chapman–Kolmogorov equations)
counts -element subsets of an -element set, and for its real value is ; Vandermonde gives . (The set of -element subsets and the binomial coefficient , for ; hence , the quotient is a natural number, and , Vandermonde's identity )
The harmonic series diverges, and positive sequences whose ratio converges to a finite positive number have the same series behavior. (For rational , converges iff , For with : if the two series share their behaviour, while and give one implication each)
A nonnegative series is the supremum of its finite partial sums; a state is recurrent exactly when its positive-time return probability is one, and the return time starts at . (Series in the nonnegative extended real line, Recurrent and transient states, Hitting, return, and visit times)
Under AC, for a fixed state of a countable-state chain, (Equivalent criteria for recurrence and transience)
Proof
Proof technique: count finite move words using the matrix Chapman–Kolmogorov equations, then apply the statewise Green-series criterion.
The quotient map from [F1] is onto. By [F2] there is a bijection ; for each , injectivity and surjectivity give a unique pair with , so assigning that unique pair defines a map . The composite is onto: for , choose a pair with , and then . Hence [F2] makes at most countable, and [F3] makes at most countable. It is nonempty, since .
For each , the four summands in are probability measures by [F4]; their weighted sum is a measure, has total mass , and is measurable in because the source sigma-algebra is the full power set [F5]. Hence is a probability kernel. Its four neighbors are distinct and its singleton entries are at those neighbors and zero elsewhere, agreeing with the matrix in [F6].
For each fixed , AC [A1] and [F7] therefore give the canonical chain law with and kernel ; [F8] identifies its transition matrix and iterates. This verifies the chain hypotheses for [F14].
Let . For any and , times the number of words with . At this is the identity-matrix statement [F8]. If it holds at , [F9] writes . By [F6] only the four possible predecessors , , contribute; grouping -step words by their endpoint and appending the unique final step counts each -step word exactly once. Each added factor is , proving the formula by induction.
Fix . A word of length returns to its starting point exactly when, for some , it contains up-steps, down-steps, and steps in each horizontal direction. For this , choose the up, down, and left positions in succession; [F10] gives The equalities follow by applying the real closed formula in [F10] to each coefficient.
Summing the counts from step 3.1 over , Vandermonde [F10] gives The formula includes , where the empty word has weight one. It is independent of . For odd length, each move flips the parity of the sum of the two coordinates, so .
Set and for . By step 4.1 and [F11], Indeed, writing gives . All are positive by step 4.1.
The harmonic series is after the index shift , and diverges by [F12]. The positive finite limit in step 5.1 and the limit-comparison theorem [F12] imply .
Every return term is nonnegative. Therefore the full partial sum dominates ; the latter is unbounded by step 6.1. By [F13] the full Green series diverges. This argument does not mistake the identity term for a positive-time return.
The fixed state space contains and at least the distinct states and , so empty and one-state cases do not occur. Every row has four positive entries; off-neighbor entries are zero, odd-time return entries vanish by step 4.1, and is included only in the Green series, not in . There is no boundary parameter, absorbing state, deterministic row, or iff claim. The one-way recurrence conclusion uses only the Green-divergence-to-recurrence direction of [F14].
For each fixed , the statewise recurrence criterion [F14] and step 7.1 show that is recurrent. By [F13] this means exactly . Since was arbitrary, every state of the two-dimensional simple symmetric walk is recurrent. AC is used to obtain the canonical laws and to apply the recurrence criterion; the finite word count, Vandermonde identity, asymptotic comparison, and parity argument require no choice.
Source notes
Durrett, Probability: Theory and Examples, 5th ed., §5.4 Example 5.4.2, Theorem 5.4.3 and complete proof, and the part of Theorem 5.4.4, printed pp. 288–289/PDF pp. 295–296 (official PDF parser lines 19421–19505), gives the return-series criterion, four-direction path count, Vandermonde reduction, and harmonic-order asymptotic. Its random-walk setup uses iid uniform increments; the item constructs the corresponding matrix chain and its canonical laws locally.
Levin–Peres–Wilmer, Markov Chains and Mixing Times, 2nd ed., §21.1 Proposition 21.3 and complete proof, and Example 21.5, printed p. 292/PDF p. 308, give the Green-series criterion and an alternate corner-walk proof. Proposition 21.3 assumes irreducibility; the corner walk's communicating-class issue is resolved in the source by the rotation/dilation observation. This item does not depend on that result: it uses the library's statewise criterion and directly computes the same return series from every starting state.
Higher-dimensional simple symmetric walks are transient
Statement
Assume AC (The Axiom of Choice). For every integer , define the probability kernel on by where are the standard basis vectors of . For each , let be the canonical path-space chain law with initial measure and transition kernel . Then every state is transient for this simple symmetric nearest-neighbor walk.
Facts & Assumptions
Given: AC, an integer , the lattice , the kernel , and a fixed initial state .
AC is assumed for the canonical path-space law and the statewise recurrence criterion used below. (The Axiom of Choice)
A Dirac set function is a probability measure; finite nonnegative weighted sums of measures are measures. (A Dirac set function is a probability measure, Nonnegative scalar multiples and countable weighted sums of measures are measures)
A probability kernel is a measure in the target variable for each source point, has total mass one, and is measurable in the source point for each measurable target set. (Measure kernel and probability kernel)
From any probability measure and probability kernel, AC supplies a unique canonical path-space law whose coordinates form the corresponding homogeneous Markov chain. (Canonical Markov chain on path space)
With initial measure , write for the specified deterministic-start chain law. (Initial distribution of a Markov chain)
The simple symmetric walk has one-step matrix for and zero elsewhere; each row sums to one. (Simple symmetric walk on the integer lattice)
The matrix probabilities are and , with . (Transition matrices and n-step probabilities)
Matrix Chapman–Kolmogorov holds: (Matrix Chapman–Kolmogorov equations)
is at most countable: it is a surjective image of . ( is countably infinite, Remark)
Every finite power of an at most countable set is at most countable. (Every finite power of an at most countable set is at most countable)
For , the multinomial coefficient counts ordered blocks of sizes , and The multinomial expansion holds for real variables. (The multinomial coefficient as the number of ordered partitions of an -set into blocks of prescribed sizes, The multinomial coefficient equals , and in )
If positive reals have nonnegative real weights summing to one, then . (The weighted arithmetic-geometric mean inequality for real weights)
Stirling's formula gives (Stirling's formula for factorials)
Every nonempty finite subset of has a maximum and minimum. (The nonempty finite subsets of are exactly the listable ones)
For rational , the series converges. (For rational , converges iff )
If nonnegative terms are eventually bounded above by terms of a convergent series, their series converges. (If eventually, convergence of gives convergence of , and divergence of gives divergence of )
For every specified chain law, means is recurrent, while means it is transient; these alternatives exhaust all states. (Recurrent and transient states)
Under AC, recurrence of a fixed state is equivalent to divergence of its return Green series: (Equivalent criteria for recurrence and transience)
Proof
For fixed , is the finite weighted sum of the Dirac probability measures at , , with coefficient . By [F1] it is a measure, and its total mass is . For fixed , the function is measurable because the source sigma-algebra is the full power set. Thus [F2] makes a probability kernel. The vectors are pairwise distinct, so its transition matrix is exactly [F5]. [F1, F2, F5, given] 1.2 By [F3], [F4], and [A1], for each fixed there is a canonical Markov chain law with this matrix and initial state . Also [F8] and [F9] show that its state space is at most countable, as required by [F18]. The law is unique for each , so no family of laws is selected by choice. [A1, F3, F4, F8, F9, given] 1.3 Repeatedly apply [F7] to the finite-support one-step rows. Induction on the number of steps expands as the sum of the probabilities of all length- move words that start and end at ; each such word has probability equal to the product of its one-step entries [F5]. At every finite time only finitely many words occur, since there are choices at each step. In particular, a return after an odd number of steps is impossible: each move changes the parity of the sum of the coordinates. [F5, F6, F7, given] 1.4 Fix and let For define where the second equality follows from [F10]. By the real multinomial expansion [F10], evaluating all variables at gives The index set is finite by [F10], and each . [F10, given] 2.1 The maximum exists by [F10] and [F14]; the set is nonempty, for example belongs to it. If for coordinates , transferring one unit from coordinate to coordinate produces and Consequently any maximizing tuple has coordinates differing by at most one. Writing with , such a tuple has coordinates equal to and the others equal to ; all such tuples have the same value. [F10, F14, step 1.4, given] 2.2 A -step word returns to zero exactly when, for each coordinate , it uses and equally often. Write their common count as ; then . For fixed , the number of words is the multinomial coefficient with the category counts , so [F10] and [F5] give its return probability as Summing over and using the definition of yields Indeed, each summand on the right is the word probability just computed. [F5, F7, F10, step 1.3, step 1.4, given, algebra] 3.1 The limit in [F12], and positivity of its terms for , imply constants such that for every integer , For fixed and , a balanced tuple has every coordinate . Put for . These positive weights sum to one; applying weighted AM–GM [F11] to gives and raising to the th power yields Use the upper Stirling bound for and the lower one for each in the factorial formula for . Since , the exponential factors cancel, and the last display gives For , [F10] gives ; increasing the constant therefore produces with Here may depend on the fixed dimension . [F10, F11, F12, step 2.1, step 1.4, given, algebra] 4.1 Since , normalization [step 1.4] gives By [F13] there is a constant with for all . Combining the return factorization, the bound from step 3.1, and the square-sum estimate just proved, there is a constant such that The odd-time return probabilities vanish by step 1.3. [F13, step 1.3, step 1.4, step 3.1, step 2.2, algebra] 5.1 For fixed integer , the rational exponent exceeds one, so [F15] gives convergence of . The comparison theorem [F16] and step 4.1 show that The initial term is one by [F6]. [F6, F15, F16, step 1.3, step 4.1, algebra] 6.1 The Green-series criterion [F18] implies that is not recurrent; [F17] gives the exhaustive recurrent/transient alternatives, so is transient. For every , translation by is a probability-preserving bijection from the finite move words from back to to the words from back to . Therefore for every , and the same finite Green-series criterion makes each transient. [F5, F6, F17, F18, step 1.3, step 5.1, given] 7.1 The time-zero return contributes exactly one; all odd positive returns have probability zero; and the estimates apply at the threshold , where the bounding exponent is . The constant is allowed to depend on fixed , so no uniform-in-d claim is made. AC [A1] is used for the canonical chain law and recurrence criterion; the path counting, finite maximization, and translation argument require no choice. The assertion is one-way, not an iff statement.
Source notes
Durrett, §5.4, Example 5.4.2 and the complete proof of Theorem 5.4.4, printed pp. 288–290 (official fifth-edition PDF at https://sites.math.duke.edu/~rtd/PTE/PTE5_011119.pdf). The theorem states the same transience classification. Its proof counts the d=3 return words, writes the return probability as a central-binomial factor times a sum of squared multinomial masses, bounds that sum by the largest mass, locates the maximum at balanced counts, and uses Stirling's formula for an maximum mass. It then handles using the embedded three-coordinate walk. The proof here extends the coefficient calculation to each fixed by weighted AM–GM and the Stirling ratio, and applies the already authored statewise Green-series criterion. The source passage does not prove this all-d coefficient estimate, and no local central limit theorem is used.
Nonnegative kernel action and finite drift
Definition
Let be a transition matrix on countable and let . Define the nonnegative kernel action
using the extended nonnegative sum of Series in the nonnegative extended real line. Terms with zero transition weight are omitted: The extended real line , its order, and the arithmetic that is left undefined leaves undefined, while each displayed product has positive finite first factor and is defined even when . If is finite-valued and , its drift is the finite real number
This agrees with the published discrete generator Discrete generator of a countable-state transition matrix on bounded functions. For an extended-valued , write a first-step relation as in extended nonnegative arithmetic; do not define a drift by subtracting from .
First-step equations for nonnegative exit costs
Statement
Assume AC (The Axiom of Choice). Let be a Markov chain on an at most countable state space with transition kernel and transition matrix . Let , put , and let and be bounded. Define the boundary payoff by when and when , so no value is used. For , let with the empty sum equal to . Then where is the support-restricted nonnegative kernel action of Nonnegative kernel action and finite drift. The equation on is in extended nonnegative arithmetic and may have value .
Facts & Assumptions
Given: AC, a countable-state Markov chain with kernel , , bounded nonnegative and , and .
The Axiom of Choice states that every family of nonempty sets has a choice function; it is assumed here for the canonical laws and conditional-expectation/Markov suppliers cited below. (The Axiom of Choice)
, so when the initial state is in . (Hitting, return, and visit times)
The infimum of the empty set is . (Hitting, return, and visit times)
for the transition matrix. (Transition matrices and n-step probabilities)
for nonnegative , with zero weights omitted. (Nonnegative kernel action and finite drift)
For bounded product-measurable , is measurable and almost surely. (Markov property for bounded future path functionals)
For bounded measurable , almost surely, where . (Bounded-function form of the Markov property)
When the initial state is fixed at , and ; hence almost surely under . (Initial distribution of a Markov chain)
On a countable discrete space, a measure is the sum of its singleton weights; for they are . (Every measure on a countable discrete space is its weighted sum of Dirac measures)
Increasing sequences of nonnegative measurable functions pass to the limit under the nonnegative integral. (Monotone convergence for the integral)
The nonnegative integral is additive, including when one or both integrals are infinite. (Additivity of the nonnegative Lebesgue integral)
Restricting a nonnegative measurable function to a measurable event by setting it to zero off the event preserves measurability. (Closure properties of measurable functions used by the integral)
A nonnegative extended series is the supremum of its increasing finite partial sums. (Series in the nonnegative extended real line)
Pointwise increasing limits of measurable functions are measurable. (Closure properties of measurable functions used by the integral)
Every nonnegative measurable function is the pointwise increasing limit of nonnegative simple functions. (Every nonnegative measurable function is the increasing limit of simple measurable functions)
For a nonnegative simple on disjoint measurable sets, its simple integral is . (The integral of a nonnegative simple function)
For a nonnegative double sequence, the two iterated sums agree, including when their common value is . (Tonelli's theorem for double series of nonnegative extended real numbers)
For bounded real , . (Basic algebra and order properties of conditional expectation)
Sums of measurable extended-real functions are measurable whenever the sum is defined pointwise. (Closure properties of measurable functions used by the integral)
For a nonnegative simple measurable function, its nonnegative Lebesgue integral equals its simple integral. (The nonnegative integral agrees with the simple integral on simple functions)
The nonnegative Lebesgue integral is the supremum of the simple integrals of all nonnegative simple minorants. (The nonnegative Lebesgue integral)
A nonnegative simple measurable function has finite range. (Nonnegative simple measurable functions)
For every and , , so the hitting events used here are measurable. (Hitting, return, and visit times)
Proof
On , put , extend by zero on and by zero on , and define , , and . The hitting events are measurable by [F22], the restrictions by [F9], the nonnegative series by [F10], and their sum by [F16]; thus is measurable, on by [F17], and no coordinate at infinity is evaluated.
If , then almost surely under by [F5], so by [F1], and ; hence . This includes an empty and a start already on the boundary.
If , then every path starting at has ; its shifted path exits at time when and never exits when , so in extended nonnegative arithmetic. Additivity [F8] gives without subtraction, also when the tail expectation is infinite.
For , let and ; then is measurable and bounded by by [F3], and its conditional future-path identity at time , followed by [F15], gives .
The bounded one-step identity [F4], expectation preservation [F15], and under [F5] give .
For a nonnegative simple with disjoint measurable , [F19] identifies its nonnegative integral with its simple integral [F13], and countable singleton weights [F6] give . For general nonnegative measurable , choose simple by [F12]; MCT [F7] passes the integrals to the limit, while [F20] fixes the nonnegative integral and [F21] ensures the increments are finite-valued nonnegative simple functions. Thus with ; Tonelli [F14] interchanges the increment and state sums when is countably infinite, using its fixed enumeration, while for finite the limit passes through the finite sum. It follows that , the support-restricted action [F18].
As , and for every ; [F7] and measurability of the increasing limit [F11] give by steps 1.4–1.6 and [F2]. Combining with step 1.3 proves on , including the value .
If , there is no probability law of an -valued chain and no state to check; if , step 1.2 covers every state; if , the boundary payoff is zero and the equation still holds when and . If , then ; a one-state absorbing chain in with positive cost has , and deterministic rows obey the same shift calculation. The endpoint is handled in step 1.2, whereas on one has and the exit-time cost is excluded by . AC [A1] is used for the canonical laws and conditional-expectation/Markov identities [F3]–[F5], [F15]; countability supplies the fixed row representation, with no additional choice principle. The two equations form no biconditional.
Superharmonic majorants bound exit costs
Statement
Assume AC (The Axiom of Choice). Let be a Markov chain on an at most countable state space , with transition matrix , let , and put . Let and be bounded. Define on and on , and put as in First-step equations for nonnegative exit costs. Suppose is finite-valued, for every , on , and on , where are the kernel action and finite drift from Nonnegative kernel action and finite drift. Then
Facts & Assumptions
Given: AC, a countable-state Markov chain, , and a finite-valued nonnegative satisfying the displayed boundary and drift inequalities and at each state.
AC supplies the canonical chain laws and the conditional-expectation versions used by the Markov and conditional-monotone-convergence results. (The Axiom of Choice)
; in particular for an initial state in , and is measurable from the first states. (Hitting, return, and visit times)
For the transition kernel , . (Transition matrices and n-step probabilities)
Under the deterministic-start law, almost surely and its expectation is denoted by . (Initial distribution of a Markov chain)
The exit reward is , with boundary payoff zero when ; its expectation is . (First-step equations for nonnegative exit costs)
is the sum over positive transition weights, and if is finite-valued with finite , then . (Nonnegative kernel action and finite drift)
Bounded measurable satisfies almost surely. (Bounded-function form of the Markov property)
Increasing nonnegative conditional expectations converge to the conditional expectation of their pointwise limit, whose defining event integrals hold for every event in the conditioning sigma-algebra. (Conditional monotone convergence)
A nonnegative integral passes through an increasing pointwise limit. (Monotone convergence for the integral)
A finite-range nonnegative function has its simple integral given by its finite sum of values times the measures of their level sets; that is its nonnegative integral. (Nonnegative simple measurable functions, The integral of a nonnegative simple function, The nonnegative integral agrees with the simple integral on simple functions)
The nonnegative integral is the supremum of the simple integrals of nonnegative simple minorants. (The nonnegative Lebesgue integral)
The integral of a pointwise lower limit of nonnegative measurable functions is at most the lower limit of their integrals. (Fatou's lemma)
Nonnegative integrals are additive, including extended values. (Additivity of the nonnegative Lebesgue integral)
An at most countable set is finite or admits a listing by . (Finite, countably infinite, countable, uncountable)
A nonnegative extended series is the supremum of its finite partial sums. (Series in the nonnegative extended real line)
Proof
Fix and a finite-valued nonnegative . Exhaust finite by its finite initial subsets, or, for countably infinite , fix an enumeration and put . Each is a finite-range simple function, and the simple-integral formula plus gives , with zero weights omitted from the row action. These functions increase to , so monotone convergence and the definition of the nonnegative row series give , also for finite .
For each finite , define . By [F1], this is a finite sum of measurable nonnegative terms, equivalently using , so is measurable and finite pathwise. On , ; on , one has , , and .
For , let . It is bounded and measurable, so [F6] and step 1.1 give almost surely. As , both and increase to their untruncated values: for the row action, its supremum over and over finite row partial sums commute, and each finite partial sum converges termwise. Conditional monotone convergence [F7] therefore yields almost surely, with the right side finite at every state by hypothesis.
Fix under . Since , suppose inductively that , which makes integrable. Integrating the conditional identity from step 2.1 over by the defining event-integral property [F7] gives . On , by the drift hypothesis, and ; thus . Off the stopped quantities agree, while on their earlier cost sums agree; nonnegative additivity [F12] now yields . Induction proves finite stopped expectations without assuming global integrability of .
Put , so by [F4]. On , for every , . On , and , whose partial costs increase to . Hence pointwise without evaluating ; Fatou [F11] and step 3.1 give . Since was arbitrary, the claim holds at every state.
If , there is no state to check. If , then and the conclusion is ; if , step 4.1 applies with . When , . For a one-state chain, a boundary start has , and if its state is in then forces and . Deterministic transitions are covered by the one-step identity. A hit at incurs and then the boundary value at . AC [A1] supports the canonical laws, bounded conditional Markov identities, and conditional monotone convergence; the pathwise comparison itself uses no choice. This is a one-way bound, with no iff claim.
Source notes
Roch, Note 24 §2 equation (4), printed/PDF p. 3, defines the same exit payoff and pre-exit running cost. In §3, Lemma 24.6 and its proof state the stopped supermartingale construction, and Theorem 24.7 and its proof state the majorant conclusion. In the proof of Theorem 24.7, the displayed identity for the stopped limit at is not justified and need not hold: the limit can retain a nonzero contribution. This proof does not use that identity or the source's supermartingale convergence step. It derives finite stopped-expectation bounds with conditional truncations and obtains the result from pointwise domination and Fatou. The source's generator was initially defined for bounded functions; this item states at every state and proves the unbounded one-step conditional identity locally.
Expected exit time solves the Poisson equation
Statement
Assume AC (The Axiom of Choice). Let be a Markov chain on an at most countable state space with transition matrix as in Transition matrices and n-step probabilities. For , put and If for every , then where and the finite drift are as in Nonnegative kernel action and finite drift. In particular, the pointwise finiteness premise holds when is finite, is irreducible, and .
Facts & Assumptions
Given: AC; an at most countable state space with a Markov chain transition matrix ; a set ; and .
AC is the axiom that every family of nonempty sets has a choice function. It is explicitly assumed by the first-step theorem and the finite irreducible hitting-time lemma used here. (The Axiom of Choice)
, with the empty infimum equal to . (Hitting, return, and visit times)
The transition-matrix entries are . (Transition matrices and n-step probabilities)
With initial state fixed at , is the law with initial distribution and is its expectation. (Initial distribution of a Markov chain)
For bounded nonnegative boundary reward and running cost , the expected exit-cost function satisfies on and on in extended nonnegative arithmetic. (First-step equations for nonnegative exit costs)
The nonnegative kernel action is . (Nonnegative kernel action and finite drift)
If is finite-valued and , then its drift is the finite real number . (Nonnegative kernel action and finite drift)
The geometric-tail clause of the finite irreducible hitting-time lemma assumes a finite state space, an irreducible transition matrix, and a nonempty target . (Geometric tail for hitting in a finite irreducible chain)
Under those assumptions, the lemma proves for every state . (Geometric tail for hitting in a finite irreducible chain)
Proof
On each path, : if , exactly the indices contribute, while if , every index contributes and both sides are . The sum is empty when . Thus the path cost in First-step equations for nonnegative exit costs with boundary payoff and running cost equals , including nonexit paths.
The first-step theorem with and has expected cost by step 1.1 and [F3], so it gives on and for . [A1, F3, F4, step 1.1, given] The constant functions are bounded and nonnegative, so the theorem applies; its relation on is in extended nonnegative arithmetic:
If is finite at every state, then for each the first-step relation forces and hence . [F5, F6, step 2.1, given] Indeed, step 2.1 gives , so . Since is finite-valued, [F6] defines , and the finite-real equation gives Thus the Poisson equation is well-defined at every state of .
If is finite, is irreducible, and , then is nonempty. Thus [F7] holds with this target, and [F8] gives for every . Steps 2.1 and 3.1 give the asserted boundary values and equation. The nonempty-target condition matters: for in a nonempty state space, , so the global finite-mean premise fails.
If , the initial-distribution definition supplies no probability law of an -valued chain; there are no states to check. If , then from every state, so and the equation on is vacuous. For a one-state chain , this is the finite irreducible proper-domain case; if instead , then and the finite-mean premise fails. As a deterministic-row check, on a finite deterministic cycle and a proper , the nonempty target is reached within at most steps; at an interior state with successor , the first-step identity reads , hence . The endpoint is counted by the empty path sum, and for one has , so the unit cost counts precisely the steps strictly before exit. AC is used through the cited first-step and finite hitting-time results; no further choice is made here. This corollary states implications, not an iff.
Lyapunov drift bound for hitting times
Statement
Assume AC (The Axiom of Choice). Let be at most countable with sigma-algebra , let be a probability kernel, and set . For each , let be the canonical path-space chain law with initial measure and transition kernel , and let be its expectation. For , define . If is finite-valued with for every and on , using the support-restricted kernel action and finite drift, then for every . Consequently .
Facts & Assumptions
Given: AC, an at most countable state space , a probability kernel with transition matrix , a target , and a finite-valued nonnegative satisfying everywhere and on .
AC is the assumption available to construct each fixed-start canonical law and is assumed by the prior first-step and superharmonic-majorant theorems. (The Axiom of Choice)
An at most countable set is finite or countably infinite. (Finite, countably infinite, countable, uncountable)
A probability kernel is a probability measure in the target variable and has total mass one. (Measure kernel and probability kernel)
For , the Dirac set function is a probability measure. (A Dirac set function is a probability measure)
AC gives the canonical path-space law for a probability initial measure and a probability kernel; its coordinate process is the corresponding Markov chain. (Canonical Markov chain on path space)
With initial state fixed at , write for the law with initial distribution and for its expectation. (Initial distribution of a Markov chain)
, the infimum of the empty set is , and when the start is in . (Hitting, return, and visit times)
The transition matrix is . (Transition matrices and n-step probabilities)
For finite-valued , ; when this is finite, . Zero transition weights are omitted. (Nonnegative kernel action and finite drift)
For bounded nonnegative boundary payoff and running cost , the first-step exit cost is , where on and on . (First-step equations for nonnegative exit costs)
If , and are bounded, and finite-valued satisfies everywhere, on , and on , then the corresponding exit cost obeys . (Superharmonic majorants bound exit costs)
Expectation of a nonnegative measurable random variable is its extended nonnegative integral, and the nonnegative integral preserves pointwise order. (Expectation of a nonnegative or integrable random variable, Monotonicity and nonnegative homogeneity of the nonnegative integral)
Proof
Fix . By [F2] and [F3], and satisfy the kernel and initial-measure hypotheses of [F4]; AC [A1] therefore supplies the canonical law , and [F5] fixes the notation . This is done for each separately, without selecting path-space realizations as a family.
Pathwise, if then exactly the indices satisfy , while if every does; hence in . In particular the sum is empty and equals zero when the starting state is in .
Set , let be the zero function on , and let be the constant one function on . Both are bounded and nonnegative, on , and [F8] identifies the given drift condition with on . Countability and the matrix-kernel relationship are [F1], [F2], and [F7].
For the exit problem in step 1.3, the boundary payoff is zero on both and , and the accumulated running cost is . By [F9] and the pathwise identity in step 1.2, its value is , including the value if the target is never hit.
The hypotheses of [F10] hold for , , and : the chain is countable by [F1], AC [A1] is assumed, step 1.3 verifies the boundary and drift inequalities, and is finite everywhere by hypothesis. Therefore step 2.1 and [F10] give .
For each integer , pointwise . By [F11] and step 3.1, ; letting grow forces . Thus the stated expectation bound also gives almost-sure hitting.
If , then and the bound is immediate. If and , step 2.1 would give , so no can satisfy the hypotheses; the implication is vacuous in this case. For a one-state chain, is the first case, while for its sole row has and , contradicting the drift assumption. On a deterministic row , the drift inequality gives until the hit, so nonnegativity prevents an infinite path outside ; zero-weight terms are omitted by [F8]. The endpoints and were handled in steps 1.2 and 2.1. AC is used for the canonical laws and the two prior theorems, not for the pathwise identity or deterministic calculation. This is a one-way bound, not an iff claim.
Source notes
Roch, Note 24 §2 equation (4), printed/PDF p. 3, defines the boundary payoff and accumulated pre-exit cost; the complete proof of Theorem 24.4, printed/PDF p. 4, supplies the first-step cost identity. Section 3 Theorem 24.8 and its complete proof, printed/PDF p. 7 (official PDF parser lines 312–336), state the Lyapunov hitting-time bound and reduce it to Theorem 24.7 with , , and . Roch assumes proper and states a nonnegative without separately requiring finite ; §1 initially defines the generator for bounded functions. This item uses the earlier library superharmonic-majorant theorem, whose explicit finite- condition makes the action and drift well-defined, and handles directly. No source uncertainty remains for the stated library claim.
5 · Examples, counterexamples and false statements
None yet.