After substituting A ~d for A and dividing by Md 'A' with a= (d I)/ d, we have
O(Md,k)/(Md A)'O(A)/A', m1. (4.2)
Now, given any E > 0 and k > 0 we can choose an interval (a, b) (a (E, k), b (E, k)) such that for all A c (a, b) we have
(p (A)/ A E + inf (p (u)l u'. (4.3)
k
Applying (4.2) to (4.3), we find
O(Md A)/ (mA)' E + inf 0 (u)l u' (4.4)
u k
for all m and A E (a, b), hence
0 (x)l x' c + inf 0 (u)l u' (4.5)
A~k
for all X E: (Md a, Md b)=U. For ma' 1d 1(b 11d a 11d) the intervals
(Md Md +1)d (M+I)d d
a, b) and ((m a, b) overlap, so U contains (mo a, oo) where %
is the least integer as great as a' 1d / (b'ld a 11d). We can thus conclude from (4.5)
that
litn sup O(A)/A' lim infO(A)/A' + e. (4.6)
A~ A0
Since (4.6) holds for all E > 0, the limit of O(A)/A' exists as A 00.
Now, if we let
s. = ES. = ES(Xl, X2,. . ., XJ, (4.7)
the asymptotics we have established for (fi(A) can be used to obtain the asymptotics of s,. If we expand 15(A) by conditioning on N, we find
'0
(P(A) E(S(Xl,X2,...,X.))P(N=n)=e' s.A"1n!, (4.8)
n=0
so we have
(P(A)=eA 1 s,A"In!cA'. (4.9)
n=0
i
i
136 J.M. Steele /Random sernimatchings
The extraction of the asymptoties of sn from that of O(A) can be achieved by appeal to classical Tauberian theorems, or by completely elementary means. We will pursue the latter route, but first we need to verify that sn is reasonably smooth. We use 11 Y11, = (E Y')'11 to denote the L' norm of E
Lemma 4. There is a constant a, depending only on d such that for independent, uniformly distributed random variables X,, the variables Yn= d,(Xn, ; Xl, X2, .. . , Xn) satisfy
11 Yn 11, ,,,(pln)~l" (4.10)
for all n 1. Consequently, we also have r 'n h n,
fo 2 2
lsn Sn+d < ad211eln 1/d lhi. (4.11)
Proof. We first bound P(Y,, y) by conditioning on Xn, ~ and applying geometric considerations. For any 0 < y < 1 and for all X E [0, 1]d = Q, we have the elementary geometric bound
P(IXi xl y) 1 2 dOdyd' (4.12)
where Wd is the volume of the unit sphere in R d . To see why the factor 2 d is needed, just note that (4.12) becomes an equality if x is one of the corners of the cube.
Since {Yn y} if and only if at most one of the events Ai = fiXi xl
Yn Y) (1 d2 dyd)n + nWdyd (1 2d(Odyd)1 (bn(y), (4.13)
and, for 1 Y d 1/2 we have P(Y, y) bounded by On (1). Naturally, ^ Y, y) = 0
1/2
if y d
If we multiply these bounds by pyP', apply the bound (1 x) e', and integrate using 1 y` e Oyd dy = d 'fl "ldr(a 1d) we can complete the proof of (4.10) by
0
applying the bound I'(x) x'.
To prove (4.11), we only have to note by (4. 10) and the restrictions on h that
S~ Sn+h ad 1 2 11d k 11d '< ad 2 11d n 11d lhi. [1
nihik
The preliminaries are out of the way, and we can now establish the main result of this section.
Lemma 5. There is a constant Cd > 0, such that as n 00,
(dl)ld
s, cdn (4.14)
J. M. Steele / Random senflmatchings 137
Proof. We first recall a classical bound on the tail of the Poisson distribution (see, if 1< _Y<2
e.g., Hardy, 1949, p. 170); 2 3 then, as A 00,
e'A/ k! = 0(exp(A (4.15)
for any 77 < 2y 1. We also note that (4.15) further implies that for each fixed 6 > 0,
1 k' e lAk IC = 0(exp(A '/2)). (4.16)
k:1 A\ ~>,\ 1
For easy checking, we will apply (4.15) and (4.16) with y and q We let A
5 6
be any positive integer and use (4.11) together with the crude bound sI, d 1/2 k to estimate s,, in terms of O(A) as follows:
(MA) = SA + Y (sl, s,) e IA k IC
k=0
= S, + 0 (A + k) e"A k 1M
( k: lkA 1 ' A3/5
+0 Y" A 3/5 A"d e"A k 1M
GlkA I
= S, + 0(exp(A 1/6 /2)) + O(A
Since P(A)= CA Id 1)1d + o(A Id111d ) by (4.9), we thus have s, = cA (dOld + o(A Id ')/') as well. The fact that cd > 0 follows from the fact that by elementary geometric probability such as applied in (4.12) one has a c> 0 such that E minj
One finds a familiar pattern in the derivation of the asymptotics of 0 (A) by means of the subadditivity argument given in equations (4.2) through (4.7). On the other hand, the use of Hardy's bound on the Poisson tails has not been used before in the context of subadditive Euclidean functionals, and the introduction of this bound provides a simpler and more powerful approach than the Tauberian arguments used in K.arp and Steele (1985) or Steele et al. (1987). From the perspective of the general theory, where,there is some benefit to working only with onesided bounds, the Tauberian arguments retain some benefits; but, where one has twosided control of s. s,,h as given by Lemma 4, the line of argument given by (4.15)(4.17) seems to be preferable.
5. Finishing the proof of Theorem 1
(dl)ld
Now that we know ES, cdn ' the asymptotic behavior of the random variable S, is essentially reduced to obtaining good bounds on the central moments E (& _ Sjk, or the tail probabilities ^ & s, 1 t).
i
1
i
1
138 J.M. Steele / Randoin semimatchings
By modifying the methods used for the TSP in Steele (1981b), one can show by means of the inequality of Efron and Stein (1981) that E(S,, Sn )2= Var Sn is Of order 0(n 121d). With such a bound on Var(Sn), one can use interpolation and a BorelCantelli argument to prove Theorem 1.
Still, a cleaner proof of a more precise result can be obtained by using a martingale argument to bound the fourth central moments E(Sn _ S~)4 . The latter approach avoids the interpolation argument, and, more pointedly, it provides for socalled complete convergence, rather than just almost sure convergence (see, e.g, Stout, 1974, or Steele, 1981b, for a discussion of the benefits of complete convergence in the context of probabilistic algorithms and of its difference from almost sure convergence).
We recall that a sequence of random variables di, 1 i n, is called a martingale difference sequence provided there is a sequence of sigma fields Fi, 1 i n, such that Fi c F,,, where di is measurable with respect to F,, and E (di 1 Fi,) = 0. The martingale differences we use are defined by
di=E(S,,1Fi)E(S.1Fi~), 1in, (5.1)
where for 1 i n we take Fi to be the sigma field generated by {X., X2,. .., XL and where FO is the trivial sigma field. Since E (Sn ~ Fn) = Sn and E (Sn 1 FO) = s,, the telescoping sum of (5.1) lets us express S. s. in terms of the di,
n
Sn _S~ di. (5.2)
Although it is not particularly easy to compute with the di, they can be made more tractable by introducing some new variables. We let Sn denote the length of the minimal semimatching of the sample with the ith point left out, i.e., S'n = S(Xl, X2,.. ., X1, Xi+l,..., Xn). One benefit of these variables is that E(S'n1Fi) = E (S'n 1 Fi ,), and thus we have
di = E (S. S'n 1 Fi). (5.3)
The critical point is that each expectation in (5.3) is well adapted to analysis by means of Lemmas 2 and 4. In fact, by (5.3) and Jensen's inequality, we have for each p 1 that
Idi1P E(JS, S'n1P1Fi), so taking expectations and using (4.10) gives
ildilip 2ad(pIn ) Ild, (5.4)
where ad, the constant of Lemma 4, depends only on d.
Now, for any martingale difference sequence, Burkholder's square function inequality (Burkholder, 1973, or Chow and Teicher, 1978, p. 384) tells us for p > 1 that
n n 1/2
di 18pq' /2 d 2
1 i
p 11 ( i = 1 ) 11 p
i
i
J. M. Steele / Random semimatchings
where I lp+llq= 1. For p= 4, we find
)4_ 2
E (1~ di _ cE d 2
i
where c 3 6 .2 16 . By expanding this last sum and applying H51der's inequality, we find from (5.4) that
( i n )4 " 4 2 2
E di cE di+2cE didj
1 i<,1 n
n
4
cE 1 di+2
i=1
Kdn 24/d
4)1/2 4)1/2
(Ed 1 (Edl
139
(5.5)
for a constant Kd depending only on d. By Markov's inequality, we then have for any e > 0 that
P(IS,, s, 1 en (d 1)l d)__ '4 Kdn 2. (5.6)
(di)/d
Thus, the probabilities in (5.6) are summable for each s > 0, and since s,, cin this summability is exactly the condition of complete convergence of sn'Sn to the constant Cd. Since the BorelCantelli lemma tells us complete convergence implies almost sure convergence, the proof of Theorem 1 is complete. E]
6. Large deviations
1~
In Section 5 we gave the quickest and cleanest route to the completion of the proof of Theorem 1. More was proved than was needed complete convergence instead of almost sure convergence but the stronger result was obtained largely because it came for free. The purpose of this section is to show how martingale theory can be used to obtain much stronger bounds on the tail probabilities of S. s,, than we found in (5.6).
We continue to exploit the representation (5.2) and, in particular, it will be used together with a recent martingale inequality to prove the exponential tail bound:
P(IS, s. 1 t) A exp( _Bdt2d1(2+d )n (2d)1(2+d) ), 1n<00, 0
where A = e and Bd is a constant that depends only on the dimension d.
Inequality (6.1) is powerful in any dimension d 2, but it is especially convenient for d= 2. In that case, (6.1) reduces to an ordinary exponential bound that is independent of n. Also, on multiplying (6.1) by pt' and integrating, we find by standard bounds on F(p) that when d = 2 all the central moments of S. are bounded independently of n, i.e.,
11 Sn S. 11, JOA
where 8 is a universal constant.
i
i
i
1
1
(6.2)
140 J.M. Steele / Rwidoin seiniinatchings
We can also exploit (6. 1) in another direction to get a rate result for Theorem 1 For example, when d =2 and we take t=2 log nI B,,, then (6.1) leads to a summable bound on the tail probabilities. By the BorelCantelli lemma, we then have a qualitative refinement of Theorem 1:
& = s,, + 0(log n) (6.3)
with probability one. One should note, however, that we cannot replace s,, with C2n 1/2 in (6.3), since we have no bound on S,,_ C"n 1/2 that is sharper than o(n' /2 )
We will now show that for any d 2 inequality (6.1) follows easily from the LP bound on di given in (5.4), and a general martingale inequality due to Rhee and Talagrand (1987). The RheeTalagrand inequality states that there is a constant K such that for any martingale difference sequence {di, 1 i n}, and any t 0 we have
P di t) exp( 2~s), (6.4)
provided s 2 and Ks (jj, 2, t 2.
di 2
When we apply our LP bound (5.4) with p = 2s in (6.4), we find
1112, 2 )2/d,
ldi 2 n4ad(2sln (6.5)
n
11 dill 2, t2,
so we have Ks(liIn 2 provided we take
s=K dl(d +2) a d 2d1(d+2 )2 (2d+2)/(d+2) n (2 d )I (d +2) t 2d/ (d +2). (6.6)
For s 2 the bound on the right in (6. 1) is at least one, so if we take & 2 3 K d I (d +2) C, d 2d/(d+2) we have (6.1) for all d2, 1n <00 and 0
The intention of this section is to give just a taste of the analytical possibilities that are opened up by martingale methods. For d = 2, inequality (6. 1) is natural and effective, but even then there are many opportunities for additional development. To see how such analyses have gone forward in the theory of the traveling salesman problem one should consult Rhee and Talagrand (1988), where a bound is given that shows for d = 2 that the tails of the TSP functional are actually subGaussian. It is not known if such bounds hold for d > 2, but some heuristic considerations suggest that in higher dimensions one would no longer have such rapid decrease of the tail probabilities.
7. Extension to general distributions
The extension of the limit theory of S. from the uniform case of Theorem 1 to the general case of Theorem 2 rests on the fact that there is a class of probability measures that is rich enough to approximate any probability measure with support in [0, 1]d, yet constrained enough to permit a localized application of Theorem 1.
i
1M. Steele / Random sernimatchings 141
These are probability measures on [0, If' with the form g(x) dx+d~l, where (1) g (x) =jail Q,, form" congruent disjoint cubes Qi with edges parallel to the axes,
and (2) the measure ~t, is purely singular (i.e., ~t,([0, 1]d) = ~c,,(A) for a measurable set A of Lebesgue measure zero). These probability measures the socalled blocked distributions were used by Beardwood et al. (1959); and since the beginning of the subject, they have remained a regular feature of extension arguments for subadditive Euclidean functionals.
It should be clear that if a functional 5 is smooth in an appropriate sense then one can carry asymptotic results for the class of blocked distributions to the class of probability measures with bounded support. The following result from Steele (1988) points out a simple continuity condition that suffices.
Theorem. Suppose Z is a measurable realvalued function on the finite subsets of [0, 1 ]", and suppose that there is a constant K not depending on n such that Z satisfies the continuity condition
(d 1)1d
IZ(Xl, X2 1 Xn) Z(X'l, X2', x,'J1 K l{i: xi 5.~ xi}l (7.1)
Further, suppose thatfor every sequence of Li.d. random variables {Xi},,i<~ distributed with a a blocked distribution ~L = ~L, + g(x) dx we have with probability one that
Z(Xl, X2,..., Xn) cdn (dl)ld f g(X)(d1)1d dx. (7.2)
One then has that with probability one,
Z(X', X X) c,n (dl)ld f(X)(dl)ld dx (7.3)
2 n f
whenever {X'i} are independent and identically distributed with respect to anyprobability measure on [0, 1]d with an absolutely continuous part given by f(x) dx. C]
It is easy to justify (7.1) for the semimatching functional. If A
{X[, X2, X2,. Xn} and B = {x,, x2,. . . , x',} then by (2.11) we have
IS(A) S(A n B)l 21 +11d d 1/2 k 11d
~A,81
11d 1/2 11d
21 d 1 k (7.4)
i k j
where j = JAI JA n B1. Applying the same considerations to S(B) S(A n B) and
adding that bound to (7.4), we find for j = JA u BI JA n BI = l{i: Xi 0 X,~}1 that
I S(A) S(B)l 2 2+1/d d 1/2 1 k_ 11d. (7.5)
l~kj
Finally, (7.1) follows from (7.5) by standard estimates.
To complete the sketch of Theorem 2 we need to indicate why (7.2) holds for blocked distributions. We first consider the purely singular case. We let A denote
1
i i
i i
142
1 M. Steele / Randorn semimatchings
the support of ~i,, and let e > 0 be given. We then divide [0, 1]d into m" cells Q such that m' is smaller than e, and a small percentage of the Qi contain almost all of the mass of ~c,. Specifically, since A has Lebesgue measure zero, we can find an m and a subset J c {1, 2, ..m"} such that
m 1 ~2 E,
IJI Emd,
and
~,, ((iu Qi :~: 8.
ei' )')
Now, by the usual feasibility considerations we have
SM 1 S(Q) + S U qi
icj Gi ),
(7.6a)
(7.6b)
(7.6c)
(7.7)
so we only need bounds on the respective sums. By (2.10) any k points in [0, fl,' have a semimatching bounded by M'I'k Id111d; so by scaling we see that if k, is the number of points of {Xj: 1 j n} in Qi then IS(Q)l 8d 112M 'I ki 1(dl)ld.
By H61der's inequality we find
Id
1 S(Qi)_1j111d 8d 1/2 M'(iI ki)
iEJ rj
1)1d
and by the direct application of (2.10) we have
S(U Qi)8d ./2 ( il ki (dl)ld
ioi Ogi)
~ E Ild 8d 1/2 n (dOld
1 (7.9)
(7.10)
Since g,(Ujj Q) ~ E, the strong law of large numbers applied to (7.10) combines with (7.7) and (7.9) to give us
lim sup n(dl)lds(Q),< 811d 8d 1/2 +8d 112E(dl)ld,
nCO
(7.11)
with probability one. Since e > 0 is arbitrary, we have proved Theorem 1 in the case that ~L is purely singular, i.e., 11,([0, 1]d) = 1.
Now we consider the purely absolutely continuous case, i.e., ~L ([0, 1]d) = 0. We let m be fixed and let Qi, 1 __ j __ Md, be the usual partition. We consider the set E of edges e of S(Q) such that e has endpoints in two different subcells, i.e., e E E if e crosses a boundary aQi for some i. This time, let k, denote the number of points of Qi that are endpoints of an edge in E. We claim that there is a Kd such that
M, m
+K,, m1k~dl)ld
S ( U` Q) 1, S (Qi) S ( U' Q)
(7.12)
i
J. M. Steele / Random semimatchings 143
The proof of (7.12) in complete detail would require repetition of some of the considerations of Section 2, but it essentially follows from the idea that one can build a semimatching on each Qi by taking the edges of the semimatching of
S(U1,11
Q) that are completely interior to Qi together with a set of at most ki edges
112
with length at most m'd ' i.e., the diameter of Q.
To bound the sum of the ki, we bound the cardinality of E. The key observation is that for each e E E we either have 1 el > x, or else an endpoint of e is within x of some aQi. Thus, if v,(x) is the number of edges in a minimal semimatching of {Xi : 1 i n} that have length at least x, and n, (x) is the number of points of {Xi: 1 i n} that are within x of aQi for some i, then
ki 2 P, (x) + nn (X). (7.13)
Since XPn (X) is bounded by Sn, Lemma 3 and H61der's inequality tell us that we have
~d 1 (dl)ld
m' k~dl)ld.< ki
(2x18d 1/2 n (dl)ld + nn (X))(d1)1d. (7.14)
When we set x = n ' /d2 a standard analysis of the right hand side of (7.14) shows it is o(n W1)1d ) with probability one. Returning to (7.12), we find
~d ~d
S U Qi 1 S(Q) o(n (dl)ld
c=1 i=l
with probability one. Since the asymptotic behavior of S(Q) is determined by Theorem 1, we have completed the proof of Theorem 2 under the assumption of absolute continuity. The proof for mixed distributions follows from the consideration of the two pure cases and standard probabilistic arguments, so those details are safely omitted.
We have thus completed our sketch of the proof of (7.2). By the continuity theorem, the proof of Theorem 2 is complete. E
8. Concluding remarks
The theory developed here brings together two streams of thought that have their origin in the theory of the traveling salesman problem. First, it is widely recognized that one of the most powerful thrusts in contemporary combinatorial optimization is the algorithmic exploitation of the geometry of special polytopes. This point is forcefully made in Crowderand Padberg (1980), Gr8tschel, (1981,1982), and Lovdsz and Plummer (1986). Second, for many purposes especially probabilistic algorithms and the probabilistic analysis of heuristics there seems to be a sustained
144 J. M. Steele / Random semimatchings
contribution to be made by the theory of subadditive Euclidean functionals that has grown out of the work of Beardwood et al. (1959), Karp (1977), Papdimitriou (1977) and Steele (1981a).
The semimatching problem arises as the simplest part of Edmonds'early program to understand the matching polytope, and thus it has a special historical distinction. Its claim on our attention is further strengthened by the fruitfulness of Edmonds' conception as developed in the investigations of Padberg and Rao (1982), Gr6tschel (1977) and Gr6tschel and Holland (1985, 1987).
The semimatching problem is also the first problem to be brought into the theory of subadditive Euclidean functionals that has its origin within the framework of linear programming. To be sure, the availability of a second geometrical interpretation made the development of the probability theory of semimatching more natural than one would have otherwise expected. Still, the geometry of semimatching is not so simple that its asymptotic theory can be obtained by offtheshelf tools. The failure of the semimatching functional to be monotone lead us to a natural extension of the theory of subadditive Euclidean functionals and, in fact, the continuity established in Lemma 4 turned out to be a condition that is in some respects even more effective than monotonicity.
Of the problems that are left unresolved by the present analysis, the most obvious ones are the determination Of Cd and the possibility of a central limit theorem. There is no subadditive Euelidean functional for which these issues have been resolved; and, despite the fact that semimatching are in some ways very well behaved, there is little hope for quick progress on these problems.
A more promising line of development lies in the direction of general weight functions. The present analysis for w, = 1x yi can be extended to w, = 1X YJ', for 0 < a < d, but it does not seem easy to deal with a = d. In that case, a natural conjecture is that with probability one we have
lim min 1 1 e 1d =C> 0, (8.1)
n~ S eES
where the minimum is over all semimatchings of {Xi, 1 i n} and the Xi are independent and uniformly distributed on [0, ]d . The conjecture (8.1) is analogous to a conjecture of R. Bland on minimal spanning trees (MSTs). Bland's conjecture came about from empirical observation of simulation experiments. Its validity has been recently established by David Aldous and the author. The limit (8.1) still offers considerable technical challenge because semimatchings cannot be obtained via a greedy algorithm, and it is that feature of the MST that proved to be essential in the resolution of Bland's conjecture.
A more conceptual shift is created when one changes to w. = d (x, y) where d is a nonEuclidean distance. Sharp geometrical facts still abound, and the investigation offers reasonable hope. Nevertheless, the subtlety of tilings that might serve in the same role as Qi raises many new issues, and the development of results analogous to Theorem 1 seems to call for a new approach.
J.M. Steele / Random semimatchings 145
Acknowledgement
1 would like to thank John Mitchell for telling me about the geometric nature of (1.1), and for providing the references to the work of Gr~tschel and Holland. 1 also
thank Michel Goemans for comments on an earlier draft.
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1