Breaking Bivariate Records
James Allen Fill

TL;DR
This paper investigates the properties of bivariate Pareto records for independent uniform observations, revealing that the distribution of records broken by a new record-setting observation is asymptotically geometric with parameter 1/2.
Contribution
It establishes a fundamental property of bivariate Pareto records, specifically the asymptotic distribution of broken records conditioned on setting a record.
Findings
Asymptotic conditional distribution is Geometric with parameter 1/2.
Provides theoretical insight into bivariate Pareto record behavior.
Enhances understanding of record-breaking processes in bivariate data.
Abstract
We establish a fundamental property of bivariate Pareto records for independent observations uniformly distributed in the unit square. We prove that the asymptotic conditional distribution of the number of records broken by an observation given that the observation sets a record is Geometric with parameter 1/2.
| 0 | 50,334 | 0.50334 |
| 1 | 24,667 | 0.24667 |
| 2 | 12,507 | 0.12507 |
| 3 | 63,35 | 0.06335 |
| 4 | 3,040 | 0.03040 |
| 5 | 1,571 | 0.01571 |
| 6 | 782 | 0.00782 |
| 7 | 364 | 0.00364 |
| 8 | 202 | 0.00202 |
| 9 | 94 | 0.00094 |
| 10 | 48 | 0.00048 |
| 11 | 24 | 0.00024 |
| 12 | 18 | 0.00018 |
| 13 | 8 | 0.00008 |
| 14 | 4 | 0.00004 |
| 16 | 1 | 0.00001 |
| 17 | 0 | 0.00000 |
| 18 | 1 | 0.00001 |
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Breaking Bivariate Records
James Allen Fill
Department of Applied Mathematics and Statistics, The Johns Hopkins University, 3400 N. Charles Street, Baltimore, MD 21218-2682 USA
[email protected] http://www.ams.jhu.edu/$\sim$fill/
(Date: January 23, 2019)
Abstract.
We establish a fundamental property of bivariate Pareto records for independent observations uniformly distributed in the unit square. We prove that the asymptotic conditional distribution of the number of records broken by an observation given that the observation sets a record is Geometric with parameter .
Key words and phrases:
Bivariate records, Pareto records, record breaking, Geometric distribution, current records, maxima, time change, Glivenko–Cantelli type theorems, asymptotics
2010 Mathematics Subject Classification:
Primary: 60D05; Secondary: 60F05, 60F15, 60G17
Research for both authors supported by the Acheson J. Duncan Fund for the Advancement of Research in Statistics.
1. Introduction and main result
This paper proves an interesting phenomenon concerning the breaking of bivariate records first observed empirically by Daniel Q. Naiman, whom we thank for an introduction to the problem considered. We begin with some relevant definitions, taken (with trivial changes) from [4; 3]. Although our attention in this paper will be focused on dimension (see [3, Conj. 2.2] for general ), and the approach we utilize seems to be limited to the bivariate case, we begin by giving definitions that apply for general dimension .
Let {\bf 1}(E)=\mbox{10} according as is true or false. We write or for natural logarithm, for binary logarithm, and when the base doesn’t matter. For -dimensional vectors and , write to mean that for . The notation means .
As do Bai et al. [2], we find it more convenient (in particular, expressions encountered in their computations and ours are simpler) to consider (equivalently) record-small, rather than record-large, values. Let be i.i.d. (independent and identically distributed) copies of a random vector with independent coordinates, each uniformly distributed over the unit interval.
Definition 1.1**.**
(a) We say that is a Pareto record (or simply record, or that sets a record at time ) if for all .
(b) If , we say that is a current record (or remaining record, or minimum) at time if for all .
(c) If , we say that breaks (or kills) records if sets a record and there exist precisely values with such that is a current record at time but is not a current record at time .
For (or , with the obvious conventions) let denote the number of records with , and let denote the number of remaining records at time .
Here is the main result of this paper.
Theorem 1.2**.**
Suppose that independent bivariate observations, each uniformly distributed in , arrive at times . Let if the observation is not a new record, and otherwise let denote the number of remaining records killed by the observation. Then , conditionally given , converges in distribution to , where G\sim\mbox{\rm Geometric(1/2)}, as .
Equivalently, the conclusion (with asymptotics throughout referring to ) is that
[TABLE]
Here is an outline of the proof. In Section 2 we provide a simple and short proof of the well-known result that
[TABLE]
where denotes the harmonic number. In Section 3 (see Theorem 3.9) we show that
[TABLE]
for all and all . The improvement
[TABLE]
to (1.1) then follows immediately, where is a first-order correction term with
[TABLE]
to the Geometric probability mass function (pmf) . This improvement shows that approximation of the conditional pmf in Theorem 1.2 by the uncorrected Geometric pmf has (for large ) vanishingly small relative error not just for fixed , but for . It also shows that the corrected approximation has small relative error for . Of course we always have , and, by [4, Rmk. 4.3(b)] we have almost surely; the corrected approximation thus gives small relative error for rather large values of indeed.
As one might expect, the correction terms sum to [math]. We observe that the correction is positive (and of largest magnitude in absolute-error terms) when , vanishes when , and is negative (and of nonincreasing magnitude) when .
Formulation of Theorem 1.2 was motivated by [3, Table 1], reproduced here as Table 1. Table 1 tabulates, for the first 100,000 records generated in a single trial, the number of records that break remaining records, for each value of . The Geometric pattern is striking. The precise relationship between Theorem 1.2 and the phenomenon observed in Table 1 is discussed in Section 4, where a main conjecture is stated and a possible plan for completing its proof is described.
Throughout, we denote the observation simply by (note: subscripted will have a different later use) and, for any Borel subset of , the number of the first observations falling in by .
2. The probability that
In this section we compute the probability (that the observation is a record) exactly and approximate it asymptotically. This result is already well known, but we give a proof for completeness.
Proposition 2.1**.**
For we have
[TABLE]
Proof.
We have
[TABLE]
Integrating, we therefore have
[TABLE]
as claimed. ∎
3. The probability that
In this section, we compute for exactly and produce the approximation (3.7) with its stated error bound.
3.1. The exact probability
Over the event (with ), denote those remaining records at time broken by , in order from southeast to northwest (that is, in decreasing order of first coordinate and increasing order of second coordinate), by . Note that if we read all the remaining records in order from southeast to northwest, then appear consecutively.
If there are any remaining records at time with second coordinate smaller than , choose the largest such second coordinate and denote the corresponding remaining record by [and note that then appear consecutively]; otherwise, set .
Similarly, if there are any remaining records at time with first coordinate smaller than , choose the largest such first coordinate and denote the corresponding remaining record by [and note that then appear consecutively]; otherwise, set .
Observe that, (almost surely) over the event , we have and . In results that follow we will only need to treat three cases: (i) and ; (ii) and ; and (iii) and . The fourth case and can be handled by symmetry with respect to the second case.
Our first result of this section specifies the exact joint distribution of . We write for the falling factorial power
[TABLE]
and we introduce the abbreviations
[TABLE]
for sums that will appear frequently in the sequel.
Proposition 3.1**.**
(i)* For and*
[TABLE]
we have
[TABLE]
(ii)* For and*
[TABLE]
we have
[TABLE]
where here .
(iii)* For and*
[TABLE]
we have
[TABLE]
where here .
Proof.
We present only the proof of (i); the proofs of (ii) and (iii) are similar. We shall be slightly informal in regard to “differentials” in our presentation. The key is that the event in question (almost surely) equals the following event:
[TABLE]
where is the following disjoint union of rectangular regions:
[TABLE]
See Figure 1. But the probability of the event (3.1) is
[TABLE]
which reduces easily to the claimed result. ∎
Remark 3.2**.**
When , Proposition 3.1 is naturally and correctly interpreted as follows:
(i) For and and we have
[TABLE]
(ii) For and and we have
[TABLE]
(iii) For and and we have
[TABLE]
To obtain an exact expression for , one need only integrate out the variables in Proposition 3.1 to get
[TABLE]
where , , and (all of which also depend on ) correspond to parts (i), (ii), and (iii) of the proposition, respectively. For small values of this can be done explicitly, but for general we take an inductive approach. To get started on the induction, we first treat the case .
3.2. The case
Using Remark 3.2, we obtain the following result.
Proposition 3.3**.**
We have
[TABLE]
and therefore
[TABLE]
Proof.
Using Remark 3.2, we perform the computations in increasing order of difficulty. First, it is clear that for . Next, for we have
[TABLE]
Finally, for we have
[TABLE]
the final equality after two integrations by part. Using the computation in the proof of Proposition 2.1 and the above computation of , for we therefore find
[TABLE]
Now just use (3.2) to establish the asserted expression for . ∎
3.3. Simplifications
The expressions obtained from Proposition 3.1 for , , and for are easily simplified by integrating out the four variables that don’t appear in the integrand (when they do appear as variables). Here is the result.
Lemma 3.4**.**
Assume . Let be defined as explained at (3.2).
(i)* For we have*
[TABLE]
(ii)* For we have*
[TABLE]
where here and if then the integral is taken over .
(iii)* For we have*
[TABLE]
where here and if then the interpretation is .
Remark 3.5**.**
Alternative expressions involving only finite sums are available for by recasting the expressions in square brackets in Lemma 3.4 as finite sums of nonnegative terms, expanding the integrand multinomially, and integrating the resulting polynomials explicitly. When this is done, one finds that are all rational, as therefore are and .
Take as an example. We have
[TABLE]
and carrying out this procedure yields
[TABLE]
where the indicated sum is taken over -tuples of nonnegative integers summing to and the natural interpretation for is . Examples include
[TABLE]
Since our aim is to compute up to additive error for large , the following lemma will suffice to treat the contributions .
Lemma 3.6**.**
For , the probabilities satisfy
[TABLE]
Proof.
Recalling that denotes the number of remaining records at time , it is clear from the description of case (iii) leading up to Proposition 3.1 that
[TABLE]
Therefore
[TABLE]
3.4. Recurrence relations
In this subsection we establish recurrence relations for and in the variable , holding fixed and treating the probabilities as known.
Lemma 3.7**.**
For we have
- (i)
* if ,* 2. (ii)
* if .*
Proof.
(i) Begin with the expression for in Lemma 3.4 and integrate out the variable . This gives
[TABLE]
with in the subtracted integral. For , observe that the variable does not appear within the square brackets in the integrand. Thus, integrating out and then shifting variable names, we find
[TABLE]
where the last equality follows from Lemma 3.4. We see also from Lemma 3.4 that . This completes the proof of part (i).
(ii) The proof of part (ii) is similar. Begin with the expression for in Lemma 3.4 and integrate out the variable . This gives (with )
[TABLE]
For , observe that the expression within equals , which doesn’t depend on . Thus, integrating out , we find
[TABLE]
where the last equality follows from Lemma 3.4. We see also from Lemma 3.4 that . This completes the proof of part (ii). ∎
The recurrence relations of Lemma 3.7 are trivial to solve in terms of the probabilities and the “initial conditions” delivered by Proposition 3.3.
Lemma 3.8**.**
For and we have
[TABLE]
Proof.
Clearly we have (3.5) and likewise
[TABLE]
Then plugging (3.5) into (3.6) and rearranging yields (3.4). ∎
3.5. Approximation to the probability , with error bound.
Theorem 3.9**.**
For and every we have
[TABLE]
Proof.
Recall from (3.2) that ; substitute for and using Lemma 3.8; then substitute for and using Proposition 3.3; and finally rearrange.
For this gives
[TABLE]
Denote the coefficient of (with ) by . Note that depends only on , and that (with equality for and ). So Lemma 3.6 gives the bound on the remainder term (with half as big a constant).
For this gives
[TABLE]
A simple argument omitted here shows that this differs from the approximation in the statement of the theorem by at most for all .
For
this together with (3.3) gives
[TABLE]
Now another simple and omitted argument shows that this differs from the approximation in the statement of the theorem by at most for all .
For we have , and another simple argument shows that this differs from the asserted approximation by at most provided , the worst case being for and for . Further, the bound can be checked directly for , the worst in each of those cases again being . ∎
Example 3.10**.**
The matrix with and is
[TABLE]
Observe that the row sums to , as noted at Lemma 3.6. The matrix with entries for the same values of and is
[TABLE]
Observe that the row sums to , as guaranteed by Proposition 2.1. The matrix with entries is therefore
[TABLE]
with every row summing to unity.
Remark 3.11**.**
(a) Not that the optimal numerical constant appearing on the right in (3.7) is important to know, but it would appear from (3.8) and other computations that the optimal constant is , achieved in four cases: with .
(b) More importantly, we do not know whether the order of the error bound in Theorem 3.9 is asymptotically optimal. While the approximation is perfect for if , for it underestimates by if , and for it underestimates by if . Thus the rate of convergence is but .
For fixed , we conjecture that the correct rate of convergence is , and more strongly that the error satisfies
[TABLE]
as . Since
[TABLE]
this suggests that perhaps the optimal rate (uniformly in ) for Theorem 3.9 is the small improvement .
4. Conjectures
The upshot of this section is that a variance bound would imply a Glivenko–Cantelli type theorem: Conjecture 4.9 would imply Conjecture 4.1.
4.1. The natural conjecture
While our main Theorem 1.2 does begin to explain how the Geometric distribution arises in connection with the breaking of bivariate records, it is not the conjecture to which one is led by performing many independent trials of generating a large number of records and, for each trial, watching the table such as Table 1 evolve as records are generated one at at a time. A natural conjecture concerns the fractions of records that break remaining records, for various values of . Accordingly, let
[TABLE]
where
[TABLE]
A strong conjecture one might form is the following, of Glivenko–Cantelli type:
Conjecture 4.1**.**
The fractions of the first records that break precisely remaining records satisfy
[TABLE]
In the remaining subsections we show how proving this conjecture can be reduced to an asymptotic variance calculation, and we leave that calculation for future research.
4.2. Uniformity in
Of course, Conjecture 4.1 would have the following corollary, of strong law of large numbers type.
Conjecture 4.2**.**
For each fixed , the fraction of the first records that breaks precisely remaining records satisfies
[TABLE]
But it is standard to check that Conjecture 4.2 also implies Conjecture 4.1. For completeness, here is a proof, with all claims holding almost surely. Let denote the random variable . Then for any we have
[TABLE]
by Conjecture 4.2. But
[TABLE]
Therefore
[TABLE]
Letting completes the proof. ∎
4.3. Time change
We show next that Conjecture 4.2 would follow from the following “observations-time” conjecture. Let
[TABLE]
where
[TABLE]
Note that
[TABLE]
and define
[TABLE]
Conjecture 4.3**.**
For each fixed we have
[TABLE]
Here is a proof that Conjecture 4.3 implies Conjecture 4.2. Working in observations-time, for , let denote the time at which the record is set, so that for all . In similar fashion, . Thus Conjecture 4.2 follows from Conjecture 4.3 simply by looking at the sequence of -values. ∎
4.4. Expectations
Conjecture 4.3 is certainly plausible, because, as we prove in this subsection, with
[TABLE]
we have
[TABLE]
In the statement of the following lemma, we refer (indirectly) to the second-order harmonic numbers
[TABLE]
(aside: we shall encounter the fourth-order harmonic numbers in Section 4.6) and (directly) to the second-order Roman harmonic numbers (cf. [5] and references [16, 22, 23] therein)
[TABLE]
The lemma shows that
[TABLE]
gives a good approximation to .
Lemma 4.4**.**
For we have
[TABLE]
and, for every , also
[TABLE]
Proof.
For (4.3), just sum the result of Proposition 2.1 (with replaced by ) over from to . For (4.4), apply the same operation to (3.7) in Theorem 3.9, observing . ∎
Remark 4.5**.**
From Lemma 4.4 it is an immediate corollary that
[TABLE]
in particular, (4.2) holds, uniformly in .
4.5. Reduction to a variance calculation
In light of Lemma 4.4, to establish as it would be sufficient to establish concentration of measure for the distributions of the denominator and the numerator of —for example, by means of variance bounds combined with Chebyshev’s inequality. As we will explain in this subsection, we already know about the variance of , and if we were to bound the variance of in suitably similar fashion we could prove not only convergence in probability but also the almost sure convergence of Conjecture 4.2.
The following results concerning are implied by [4, Thms. 4.1(b), 4.2(a)] (with the mean, variance, and central limit theorem results there taken from Bai et al. [2; 1]) after specializing to our present case of dimension .
Lemma 4.6**.**
Let denote the standard normal distribution function. The number of records set through time satisfies
[TABLE]
[TABLE]
[TABLE]
and consequently
[TABLE]
A careful review of the proof of (4.5) (a first Borel–Cantelli argument applied along a geometrically increasing sequence of times), which immediately implies (4.6), shows that to establish (4.5) it is sufficient to know that the samples paths of the process are nondecreasing, that
[TABLE]
for some constants and , that , and that
[TABLE]
Now observe, for each fixed , that the sample paths of the process are nondecreasing, that
[TABLE]
with and , and that
[TABLE]
with the last equality holding by Theorem 3.9. Thus the analogues of (4.5)–(4.6) for hold if we can establish that
[TABLE]
satisfies , which (in light of the known corresponding result for ) seems eminently reasonable to conjecture.
Conjecture 4.7**.**
For each fixed , the variance defined at (4.7) satisfies
[TABLE]
A summary of this subsection is that Conjecture 4.7 would imply Conjecture 4.3 and therefore also Conjecture 4.1.
Remark 4.8**.**
(a) Use of the refinement (4.5) to (4.6) shows that Conjecture 4.7 would imply the refinement
[TABLE]
of Conjecture 4.3 for each fixed and any .
(b) More than Conjecture 4.7, we conjecture that for each fixed we have
[TABLE]
for some constants satisfying as (likely with , letting ), and that there is asymptotic normality for . It seems reasonable to conjecture that, moreover, the random vector enjoys full-dimensional asymptotic -variate normality.
(c) It may be that the random variables are positively correlated for fixed as varies, the idea being that larger values of (more records) should lead to larger values of (more records that break remaining records) for every . If this positive correlation were to be known, then Conjecture 4.7 would follow immediately, without the need for additional calculations. Indeed, for large and fixed we would then have
[TABLE]
4.6. Reduction of the variance calculation
Corresponding to the breakdown into cases utilized in Section 3, observe that satisfies
[TABLE]
where the four terms here are the respective indicators of the events
[TABLE]
By analogy with (4.1), define respective record counts , so that
[TABLE]
It thus seems daunting to calculate to prove Conjecture 4.7. But in this subsection we argue by means of suitable control of all but the first term in (4.8) that
[TABLE]
for fixed , thus reducing proof of Conjecture 4.7 to proof of the following simpler conjecture.
Conjecture 4.9**.**
For each fixed we have
[TABLE]
Here is a proof that Conjecture 4.9 would imply Conjecture 4.7. By the triangle inequality for -norm , in obvious notation we have
[TABLE]
But, with counting the number of records through time in the first coordinate, we have
[TABLE]
and, with counting the number of observations through time that set a record in both coordinates, we have
[TABLE]
Thus, returning to (4.9) and applying the inequality , we find
[TABLE]
and so Conjecture 4.9 would imply Conjecture 4.7. ∎
Remark 4.10**.**
(a) Observe that for every , and so . For , we claim that (4.11) can be strengthened to . To establish the lower bound matching the upper bound (4.11), we perform two computations. The first, valid for , is that
[TABLE]
and the other, valid for , is that
[TABLE]
(b) We conjecture that (4.10) can be strengthened to . If we knew even the upper bound , then it would follow from (4.9) and the matching upper bound on that
[TABLE]
In that way, if one could prove the conjecture that for some constant , then the same lead-order asymptotics would apply to .
Acknowledgements**.**
We thank Vince Lyzinski, Daniel Q. Naiman and Fred Torcaso for helpful comments, and Daniel Q. Naiman for producing Figure 1.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] Zhi-Dong Bai, Chern-Ching Chao, Hsien-Kuei Hwang, and Wen-Qi Liang. On the variance of the number of maxima in random vectors and its applications. Ann. Appl. Probab. , 8(3):886–895, 1998.
- 2[2] Zhi-Dong Bai, Luc Devroye, Hsien-Kuei Hwang, and Tsung-Hsi Tsai. Maxima in hypercubes. Random Structures Algorithms , 27(3):290–309, 2005.
- 3[3] James Allen Fill and Daniel Q. Naiman. Generating Pareto records, 2019. ar Xiv:1901.05621.
- 4[4] James Allen Fill and Daniel Q. Naiman. The Pareto record frontier, 2019. ar Xiv:1901.05620.
- 5[5] J. Sesma. The Roman harmonic numbers revisited. J. Number Theory , 180:544–565, 2017.
