The answers areDistinct natural numbers have . Taking in the Cauchy sequence condition forces every sufficiently late pair of terms to be equal. Every Cauchy sequence is therefore eventually constant and converges in , proving completeness.
The sequence has no convergent subsequence, since convergence would force its sufficiently late terms to lie within distance of its limit of a sequence, hence to equal that limit. Thus sequential compactness fails.
Every singleton is an open ball of radius , so the metric topology is the discrete topology. For example, and form a separation into two nonempty open sets, so is not connected. It is consequently not path-connected either.
The answers areWrite . The given metric describes locally uniform convergence: if and only if for every fixed . Indeed,so convergence in forces . Conversely, split the defining series at : its tail is at most , and its finitely many initial terms tend to zero.
If is a Cauchy sequence in , the same single-term estimate makes it a Cauchy sequence in the supremum norm on every . The completeness of the continuous-map space in the uniform metric gives a continuous function on with uniformly there. Uniqueness of the limit of a sequence gives , so these functions define a single continuous function on . The preceding finite-head and tail argument proves . Thus the space is complete.
The constant functions have whenever . They have no convergent subsequence, so the space is not sequentially compact.
For fixed , set . On ,as . The equivalence with locally uniform convergence proves that is a continuous path for . Hence the space is path-connected and connected.
A metric space is a complete metric space if every Cauchy sequence in converges to a point of . Explicitly, the hypothesis isand the conclusion is that some satisfies .
It is a sequentially compact space if every sequence in has a convergent subsequence whose limit of a sequence belongs to .
It is a connected space if there are no disjoint nonempty open subsets of with . Here openness refers to the metric topology of .
It is a path-connected space if, for every , there is a continuous map with and . Such a map is a path. Every path-connected space is a connected space: a separation would pull back along a path joining its two sides to a separation of the interval .
A metric space is a bounded set if there is a finite constant such thatFor nonempty , this is equivalent to containment in an open ball of finite radius: the triangle inequality converts a radius bound into a diameter bound, and conversely a diameter bound gives a ball of any slightly larger radius about a chosen point.
It is a complete metric space if every Cauchy sequence in has a limit of a sequence belonging to . Explicitly, the hypothesis on isand completeness requires an with . ThusBoundedness controls distances; completeness ensures that these limiting points remain in the space.
A metric space is a compact space if every open cover , with all open in , has a finite subcover: finitely many indices cover .
It is a sequentially compact space if every sequence in has a convergent subsequence whose limit of a sequence belongs to . In formulas,A finite subcover is the defining test for compactness; a convergent subsequence is the defining test for sequential compactness.
Apply part (i) for every positive integer and discard the countable union of its exceptional null sets. A sample path bounded below never reaches for some such , and must therefore converge to a finite limit of a sequence.
Apply the same argument to the martingale . Outside one more null set, every sample path bounded above also converges finitely. Thus a sample path which does not converge finitely must be unbounded in both directions. Each finite initial segment has finite values, so removing any such segment preserves unboundedness. It follows that the limit superior is and the limit inferior is . ConsequentlyThis proves the bounded-increment martingale convergence-or-oscillation dichotomy; in particular one-sided divergence to infinity is impossible with positive probability.
Both and are increasing, so each has a limit of a sequence in . Apply part (c)(ii) to the martingale , whose bounded increments were verified in part (i).
On we would have . On we would have . Both events have probability zero by the convergence-or-oscillation conclusion. Hence the two divergence events agree up to a null set. Since means precisely that infinitely many occur,Taking probabilities proves the displayed equality in the question. This stronger agreement of events is the Conditional Borel-Cantelli lemma.
We prove the Doob-Dynkin lemma here by simple function approximation. Choose such that everywhere, and letEach is a finite-valued -measurable function and pointwise. Write its level sets as , with associated values . By part (i), choose Borel sets with . Define the Borel measurable functionsAlthough the chosen need not partition all of , their inverse images do partition , so exactly.
Apply scalar clipping to each with bounds , preserving this equality, and define . A bounded limit superior of Borel measurable functions is a finite Borel measurable function. At every the limit of a sequence exists and givesThus the factorization is exact for a bounded, exactly -measurable function. If hypotheses are instead given only up to null sets, the corresponding conclusion is a factorization holding almost surely after choosing a representative.
Every is a Borel measurable function of , by the formula involving the floor function. ThusConversely, part (i) gives the everywhere identity . For fixed , this is the pointwise limit of random variables measurable with respect to . Such a limit of a sequence is measurable, so . ConsequentlyThese are increasing-precision observations even when the first finitely many are discarded; they do not behave like the independent random variables whose tail sigma-algebra appears in Question 1(b).
Choose as the pointwise limit of a sequence of where it exists, and as zero otherwise. The convergence event and every are -measurable, so this is an exactly -measurable version, bounded by . Part (a)(ii), the Doob-Dynkin lemma, supplies a Borel measurable function on such that . Applying scalar clipping to with bounds preserves that equality and ensures everywhere.
Part (c)(ii) and the conditional expectation formula from part (b)(iv) now giveSince the indices form a countable family, these identities may be taken on one common full-probability event.
For fixed , both the slope and the displayed average are constant on the atom , whose probability is . An equality holding almost surely of these constants forces the deterministic equalitySum over . The telescoping sum givesThus the desired identity holds at every dyadic endpoint, including , without evaluating the undefined slope at .
Finally, given , take dyadic endpoints . The Lipschitz condition implies , and the bound on the Borel measurable function givesPassing to the limit of a sequence provesThis is a martingale proof of the integral representation of a Lipschitz function. It constructs a bounded Lebesgue integrable function representing the increments of , and in particular proves absolute continuity of . No prior assumption that has a derivative is needed.
The uniformly integrable martingale convergence theorem states that a uniformly integrable martingale has an integrable terminal random variable such that almost surely and in the L1 norm, andThe last identity follows by passing to the limit of a sequence in for and , using convergence in L1.
Part (b)(iii) verifies uniform integrability for , soMoreover almost surely. In this particular problem the common bound also yields convergence in Lp for every finite , including convergence in L2: the dominated convergence theorem applies to . General uniform integrability alone does not assert these higher-power conclusions.
The bounded-time optional sampling theorem says that for an integrable discrete-time martingale and a bounded stopping time , . It requires no assumption about an eventual unbounded stopping time.
Apply this theorem with , or simply take the expectation of the stopped martingale in part (ii). For we obtainSince ,The monotone convergence theorem now yields . In particular almost surely, which has been established without assuming that optional stopping is valid at .
For each sample path with finite , eventually equals . Also . The dominated convergence theorem gives . Taking the limit of a sequence in the earlier identity therefore provesFor example, initial holdings give expectation one, as the first transfer must eliminate its giver. This computes the first elimination time, rather than the later time when one player owns all tokens.
does not have sequential compactness. Take the sequenceEvery subsequence has usual limit of a sequence . If a subsequence converged in the subspace topology of the Sorgenfrey line, it would also converge in the usual subspace topology, since part (c) makes the identity function from the former to the latter continuous. Uniqueness of a limit of a sequence in the usual Hausdorff space therefore forces that limit of a sequence to be .
But is an open neighbourhood of in , and no term belongs to it. Thus no subsequence converges to in , proving the assertion.
Percolation one-arm decay rate 2026-10-06
For bond percolation on the square lattice, the one-arm probability has a root limit of a sequence . The BK boundary-splitting estimate implies that is submultiplicative for positive integers. Applying the Fekete lemma to its logarithm proves existence when ; at the rate is zero. The same rate is the root limit of the percolation two-point connection probability along a coordinate axis, by the reflection lower bound for two-point percolation.
Pointwise convergence Created 2026-09-24 Updated 2026-10-14
For a sequence of functions , pointwise convergence to a function meansIt is the ordinary limit of a sequence at each fixed input. The threshold may depend on the input. Uniform convergence instead requires one threshold for the entire domain of a function.[ref]
6.1 Pointwise and uniform convergence. Basic Analysis: Introduction to Real Analysis, Volume I by Jiří Lebl, §6.1.1, Definition 6.1.1 and Proposition 6.1.5
Consider the polynomial functions , for positive integers , on the interval . For the geometric sequence tends to zero, while . ThusEach is a continuous function, but its pointwise limit is discontinuous at one. Holding an input still hides what happens near that endpoint. The analogous even-power example on appears in the source.[ref]
For and , taking the logarithm of and dividing by the negative real number reverses the inequality:The floor function followed by adding one handles the strict inequality even when the ratio is an integer. For tolerance , the first successful indices at , , and are respectively , , and . At , fails and succeeds. At and , the error from this pointwise limit is already zero, so works. Nevertheless, grows without bound as from below. A finite list of accurate test inputs cannot establish uniform convergence.
An even sharper warning concerns integration. On , define the continuous functionsTheir supports are , with height at and value zero at both ends. Every fixed eventually lies beyond the support, and always, so pointwise convergence gives the zero function. Nevertheless, each integral is the area of a triangle: . Shrinking width compensates increasing height. Hence the limit of a sequence of these integrals differs from the integral of the pointwise limit; interchanging them requires additional conditions, such as uniform convergence preserves integrals on a compact interval.
Pointwise limit Created 2026-10-06 Updated 2026-10-14
A pointwise limit assigns to each input the limit of a sequence of function values there, on the specified domain of a function. It is unique wherever it exists, by uniqueness of the numerical limit of a sequence. Its existence supplies no common approximation rate over the domain of a function. For on , it equals zero below one and one at one; restricting to with gives the zero function.
Random-cluster inverse correlation length 2026-10-14
Positive association of random variables and translation invariance give for axis connection probabilities. The Fekete lemma applied to proves the displayed limit of a sequence and the bound . The lower single-edge conditional bound gives , so the decay rate is finite and nonnegative. It may be zero.
For a real sequence with no zero terms, the displayed equivalence follows directly by comparing with . Escape to positive infinity implies reciprocal convergence to zero, but the converse does not retain the sign: is a counterexample. If , eventually , and . This proves reciprocal convergence at a nonzero finite limit of a sequence.
Sequence Created 2026-09-24 Updated 2026-10-14
A sequence assigns a value to each position in an ordered index list. For an infinite sequence in a set , one standard convention is a function , written with . Some applications start the index at zero, and a finite sequence has only finitely many positions. Values may repeat; both order and repetition matter. [ref].
For example, begins , whereas begins . Their sets of values are both , but these are different sequences. A subsequence keeps selected positions in increasing order; the subsequence of at its even integers is the constant sequence . A tail of a sequence retains all positions from one index onward.
Sequences express successive approximations, repeated observations, and the iterates of a recurrence relation. A limit of a sequence describes where its terms eventually concentrate. Finite observations alone cannot establish that behaviour: for any positive integer , the all-zero sequence and the sequence with for and for agree through index , yet have different limits of sequences. A formula or bound controlling the entire future, such as the tail diameter of a sequence in the Cauchy sequence condition, supplies information that a finite list cannot.
Series (mathematics) 2026-10-14
A series adds the terms of a sequence in their specified order. Its infinite-sum notation is defined through finite partial sums:when the displayed limit of a sequence exists as a finite number. Otherwise the series is not a convergent series in the ordinary sense. Writing an infinite list of additions does not by itself assign it a finite sum. Cesàro summation is a different prescription, with its own definition.
Two positive series make the distinction concrete. For , the individual terms tend to zero but the harmonic series has unbounded partial sums. For , partial fraction decomposition reveals a telescoping series whose partial sums tend to one. The useful question is how much all the remaining terms can contribute together, rather than only how small the next term looks.
