On permutation-invariance of limit theorems

Size: px
Start display at page:

Download "On permutation-invariance of limit theorems"

Transcription

1 On permutation-invariance of limit theorems I. Beres an R. Tichy Abstract By a classical principle of probability theory, sufficiently thin subsequences of general sequences of ranom variables behave lie i.i.. sequences. This observation not only explains the remarable properties of lacunary trigonometric series, but also provies a powerful tool in many areas of analysis, such the theory of orthogonal series an Banach space theory. In contrast to i.i.. sequences, however, the probabilistic structure of lacunary sequences is not permutation-invariant an the analytic properties of such sequences can change after rearrangement. In a previous paper we showe that permutation-invariance of subsequences of the trigonometric system an relate function systems is connecte with Diophantine properties of the inex sequence. In this paper we will stuy permutation-invariance of subsequences of general r.v. sequences. AMS 2000 Subject classification. Primary 42A55, 42A6, 60F05, 60G09. Key wors an phrases: lacunary series, limit theorems, permutation-invariance, subsequence principle, exchangeable sequences Graz University of Technology, Institute of Statistics, Koperniusgasse 24, 800 Graz, Austria. beres@tugraz.at. Research supporte by FWF grants P24302-N8, W230 an OTKA grant K Graz University of Technology, Institute of Mathematics A, Steyrergasse 30, 800 Graz, Austria. tichy@tugraz.at. Research supporte by FWF grants P24302-N8 an W230.

2 Introuction It is nown that sufficiently thin subsequences of general r.v. sequences behave lie i.i.. sequences. For example, Révész [23] showe that if a sequence (X n ) of r.v. s satisfies sup n EXn 2 <, then one can fin a subsequence (X n ) an a r.v. X L 2 such that = c (X n X) converges a.s. provie = c2 <. Uner the same conition, Gaposhin [3], [4] an Chatterji [9], [0] prove that there exists a subsequence (X n ) an r.v. s X L 2, Y L, Y 0 such that an lim sup N (X n X) N(0, Y ) (.) N N (X n X) = Y /2 a.s.. (.2) 2N log log N N Here N(0, Y ) enotes the istribution of the r.v. Y /2 ζ, where ζ is a stanar normal r.v. inepenent of Y. Komlós [8] showe that if sup n E X n <, then there exists a subsequence (X n ) an a r.v. X L such that lim N N N X n = X = Chatterji [8] showe that if sup n E X n p < where 0 < p < 2, then the conclusion of the previous theorem can be change to lim N N /p a.s.. N (X n X) = 0 a.s. = for some X L p. Note the ranomization in all these examples: the role of the mean an variance of the subsequence (X n ) is playe by ranom variables X, Y. For further limit theorems for subsequences of general r.v. sequences an for the history of the topic until 966, see Gaposhin [3]. Since the asymptotic properties of an i.i.. sequence o not change if we permute its terms, it is natural to expect that limit theorems for lacunary subsequences of general r.v. sequences remain vali after any permutation of their terms. This is, however, not the case. By classical results of Salem an Zygmun [24], [25] an Erős an Gál [2], uner the Haamar gap conition the sequence (sin 2πn x) satisfies n + /n q > =, 2,... (.3) an lim sup N N sin 2πn x N(0, ) (.4) N/2 = N log log N N = sin 2πn x = a.s. (.5) 2

3 with respect to the probability space ((0, ), B, µ), where µ enotes the Lebesgue measure. Erős [] an Taahashi [27] prove that (.4), (.5) remain vali uner the weaer gap conition n + /n + c α, =, 2,... (.6) for 0 < α < /2 an that for α = /2 this becomes false. As it was shown in [2], [3], uner the Haamar gap conition (.3) the CLT (.4) an the LIL (.5) are permutation-invariant, i.e. they remain vali after any permutation of the sequence (n ), but this generally fails uner the gap conition (.6). Similar results hol for lacunary sequences f(n x), where f is a measurable function satisfying f(x + ) = f(x), 0 f(x) x = 0, 0 f 2 (x) x <. (.7) In this case, assuming the Haamar gap conition (.3), the valiity of the CLT N N = f(n x) N(0, σ 2 ) (.8) an of its permute version epen on the number of solutions of the Diophantine equation an + bn l = c,, l N. (.9) As shown in [], [2], [3], a sharp conition for the CLT is that the number of solutions of (.9) is o(n) for any fixe nonzero a, b, c, while the permute CLT requires the stronger boun O() for the number of solutions. Permutation-invariance of limit theorems becomes a particularly ifficult problem for parametric limit theorems, e.g. for limit theorems containing arbitrary coefficients. By a classical result of Menshov [20], from every orthonormal system (f n ) one can select a subsequence (f n ) which is a convergence system, i.e. the series = c f n converges almost everywhere provie = c2 <. The question of whether a subsequence (f n ) exists such that this property remains vali after any permutation of (f n ) (i.e., by the stanar terminology, (f n ) is an unconitional convergence system) remaine open for nearly 40 years until it was answere in the affirmative by Komlós [9]. For another proof see Alous [4]. The problem of whether every orthonormal system can be rearrange to become a convergence system is still open; for a partial result see Garsia [5]. Kolmogorov showe (see [7]) that there exists an f L 2 (0, ) whose Fourier series, suitably permute, iverges a.e. But even though the Raemacher-Menshov convergence theorem yiels a sharp a.e. convergence criterion for orthonormal series, there is no similar complete result for rearrange trigonometric series. The previous results show that permutation-invariance of limit theorems lies substantially eeper than that of the original theorems an raise the question of which limit theorems hol in a permutation-invariant form for lacunary sequences. In this paper we will prove the surprising fact that, in a sense to be mae precise, all nonparametric istributional limit theorems for i.i.. ranom variables hol for lacunary subsequences (f n ) of general r.v. sequences in a permutation-invariant form provie 3

4 that the subsequence is sufficiently thin, i.e. the gaps of the sequence (epening on the limit theorem) grow sufficiently rapily. We will euce this result from a general structure theorem for lacunary sequences prove in [6] stating that sufficiently thin subsequences of any tight sequence of ranom variables are nearly exchangeable. While this iea is simple an elementary, formulating our results is somewhat technical an requires some preparations in Section 2. The proof of our theorem will be given in Section 3. 2 Main result We start with a formal efinition of the concept wea limit theorem. Let M enote the set of all probability measures on R an ϱ the Prohorov metric on M efine by Here ϱ(ν, λ) = inf { ε > 0 : ν(a) λ(a ε ) + ε an λ(a) ν(a ε ) + ε for all Borel sets A R }. A ε = {x R : x y < ε for some y A} enotes the open ε-neighborhoo of A. A ranom measure is a measurable map from a probability space to M. The following efinition is ue to Alous [4]. Definition. A wea limit theorem of i.i.. ranom variables is a system where (a) S is a Borel subset of M; T = (f, f 2,..., S, {G µ, µ S}) (b) For each, f = f (x, x 2,..., µ) is a continuous function on R M, satisfying the Lipschitz conition f (x, x 2,..., µ) f (x, x 2,..., µ) where 0 c,i an lim c,i = 0 for all i; c,i x i x i (c) For each µ S, G µ is a probability istribution on R such that the function µ G µ is measurable (with respect to the Borel σ-fiels in S an M); an () If µ S an X, X 2,... are inepenent r.v. s with common istribution µ then f (X, X 2,..., µ) i= G µ as. (2.) For example, the central limit theorem correspons to S = {µ M : x 2 µ(x) < }, G µ = N(0, Var µ), 4

5 f (x, x 2,..., µ) = (x x Eµ)/, c,i = /2 I {i }. The theorem itself is expresse by (2.). Using the terminology of [7], we call a sequence (X n ) of ranom variables etermining if it has a limit istribution relative to any set A in the probability space with P (A) > 0, i.e. for any A Ω with P (A) > 0 there exists a istribution function F A such that lim n P (X n t A) = F A (t) for all continuity points t of F A. Here P ( A) enotes conitional probability given A. (This concept is the same as that of stable convergence, introuce by Rényi [22]; our terminology follows that of functional analysis.) By an extension of the Helly-Bray theorem (see [7]), every tight sequence of r.v. s contains a etermining subsequence. As is shown in [4], [7], for any etermining sequence (X n ) there exists a ranom measure µ (i.e. a measurable map from the unerlying probability space (Ω, F, P) to M) such that for any A with P (A) > 0 an any continuity point t of F A we have F A (t) = E A ( µ(, t]) (2.2) where E A enotes conitional expectation given A. We call µ the limit ranom measure of (X n ). The following result is Alous celebrate subsequence theorem [4]. Theorem 2. Let (X n ) be a etermining sequence with limit ranom measure µ. Let T = (f, f 2,..., S, {G µ, µ S}) be a wea limit theorem an assume P ( µ S) =. Then there exists a subsequence (X n ) such that f (X n, X n2,..., µ) G µ P. (2.3) In case of the CLT formalize above, assuming sup n EX 2 n < + implies easily that µ has finite variance almost surely an thus enoting its mean an variance by X an Y, respectively, we see that the integral in (2.3) is the istribution N(0, Y ). Hence (2.3) states in the present case that N N = (X n X) N(0, Y ) which is exactly the CLT of Chatterji [9] an Gaposhin [4] formulate in the Introuction. Theorem 2. shows that a similar subsequence theorem hols for any wea limit theorem of i.i.. ranom variables. For a version of this result for strong (a.s.) limit theorems, we refer to Alous [4]. In what follows, we change the technical conitions on f in the efinition of wea limit theorems slightly, leaing to a class more convenient for our purposes. Definition. The limit theorem T = (f, f 2,..., S, {G µ, µ S}) is calle regular if there exist two sequences p q of positive integers tening to + an a sequence ω + such that 5

6 (i) f (x, x 2,..., µ) epens only on x p,..., x q, µ (ii) f satisfies the Lipschitz conition f (x p,..., x q, µ) f (x p,..., x q, µ ) ω q i=p x i x i α + ϱ (µ, µ ) (2.4) for some 0 < α where ϱ is a metric on S generating the same topology as the Prohorov metric ϱ. Thus in this case the function f epens only on a finite segment x p,... x q of the variables x, x 2,.... On the role of ϱ see [4]. The above efinition brings out clearly the crucial feature of limit theorems, namely the fact that the valiity of the theorem oes not epen on finitely many terms of (X n ), while the original efinition assumes only that the epenence of f (X, X 2,...) on any fixe variable X j of the sequence is wea if is large. However, there is very little ifference between these assumptions. For example, the central limit theorem can be formalize by either of the functions f (x,..., x, µ) = (x x Eµ)/ an f (x [ /4 ],..., x, µ) = (x [ /4 ] x Eµ)/ of which the secon leas to a regular limit theorem with the Wasserstein metric ( /2 ϱ (µ, µ ) = Fµ (x) F µ (x) x) 2, 0 where F µ, F µ enote the istribution function of µ an µ, respectively. Uner boune secon moments, the contribution of the first /4 terms in the norme sum efining f are irrelevant an thus we can always switch from f to f an bac again. The same proceure applies in the general case. We are now in a position to formulate the main result of our paper. Theorem 2.2 Let (X n ) be a etermining sequence with limit ranom measure µ. Let T = (f, f 2,..., S, {G µ, µ S}) be a regular wea limit theorem an assume that P ( µ S) =. Then there exists a subsequence (X n ) = (Y ) such that for any permutation (Y ) of (Y ) we have f (Y, Y 2,..., µ) G µ P. (2.5) Note that we assume the regularity of the limit theorem, but as we pointe out before, this is no restriction of generality. The limit theorem T in Theorem 2.2 is nonparametric, i.e. the function f epens on x, x 2,... an µ, but on no aitional parameters. A simple example of a parametric istributional limit theorem is the weighte CLT, where f = A a j (x j Eµ), A = j= 6 j= a 2 j /2.

7 For any fixe coefficient sequence (a ) this efines a nonparametric limit theorem T an Theorem 2.2 applies, but the selecte subsequence (X n ) epens on (a ). As the iscussion above shows, in the case of a parametric limit theorem T eciing whether a universal subsequence (X n ) woring for all parameters is generally a very ifficult problem; an example of a limit theorem where such a choice is impossible is given in [6]. For this reason, in the present paper we eal only with nonparametric limit theorems. In Alous [4] a formalization of strong limit theorems is also given an the analogue of Theorem 2. is prove. Using a reformulation of strong limit theorems as a sequence of probability inequalities as given in [5], [6], a version of our Theorem 2.2 can be given for a subclass of limit theorems consiere in [4]. We also mention that for a more limite class of wea limit theorems Theorem 2.2 was prove in [2]. 3 Proof of Theorem 2.2. To simplify the formulas, let f (µ) enote, for any µ S, the istribution of the ranom variable f (ξ, ξ 2,..., µ) where ξ, ξ 2,... are inepenent r.v. s with common istribution µ. The following statements are easy to verify: (A) If ϱ(µ, ν) ε then ϱ(f (µ), f (ν)) ε α q + ϱ (µ, ν) where α, q an ϱ are the quantities appearing in (2.4). (B) Let µ,..., µ r an ν,... ν r be probability istributions, further let c,..., c r be nonnegative numbers with r i= c i =. Assume that the sum of those c i s such that ϱ(µ i, ν i ) ε is at most ε. Then the Prohorov istance between r c i ν i is at most 2ε. i= r i= c i µ i an (C) Let µ an ν be ranom measures (i.e. measurable maps from a probability space (Ω, F, P) to M) such that P (ϱ( µ, ν) ε) ε. Then the Prohorov istance between µp an νp is 2ε. To prove statement (A) note that if ϱ(µ, ν) ε then by a theorem of Strassen [26] there exist, on some probability space, r.v. s ξ an η with istribution µ an ν such that P ( ξ η ε) ε. On a larger probability space, let (ξ n, η n ) (n =, 2,...) be inepenent ranom vectors istribute as (ξ, η). Clearly P ( ξ i η i ε) ε (i =, 2,...) an thus using (2.4) we see that f (ξ p,..., ξ q, µ) f (η p,..., η q, ν) ε α q + ϱ (µ, ν) except on a set with probability εq ε α q, proving (A). (Clearly we can assume 0 < ε an that in the efinition of regular limit theorems we have ω for all.) Statements (B) an (C) are almost evient, (B) is a special case of (C). To prove our theorem, let (X n ) be a etermining sequence of r.v. s with limit ranom measure µ. Then (X n ) is tight, i.e. sup j P ( X j t) 0 as t. As ω +, we can choose a nonecreasing sequence (r ) of integers tening to + so slowly that r min(p, ω /4 ) (3.) 7

8 an ( sup P X j ) j 2 ω/(4α) Let (ε ) ten to 0 monotonically an so rapily that 2 r 2 ( ). (3.2) ε α r q. (3.3) Using the structure theorem [6, Theorem 2], it follows that there exists a subsequence (X n ) an a sequence (X ) of r.v. s such that X n X = O(2 ) a.s. (3.4) an X has the following properties: (A ) Each X taes only finitely many values (B ) σ{x } σ{x 2 }... (C ) For each the atoms of the finite σ-fiel σ{x r } can be ivie into two classes Γ an Γ 2 so that A Γ P (A) ε r (3.5) an for any A Γ 2 there exist i.i..r.v. s {Z (A) j, j = r +, r + 2,...} efine on A with istribution function F A such that P A ( X j Z (A) j ε r ) εr j = r +, r + 2,.... (3.6) Here F A enotes the limit istribution of (X n ) on the set A (which exists since (X n ) is etermining) an P A enotes conitional probability with respect to A. Let µ n enote the ranom measure efine by µ n (B) = E( µ(b) X n). By Lemma 7 of [6] we have µ n µ a.s. an thus by passing to a further subsequence of (X n ) we can also assume that P {ϱ( µ n, µ) ε n } ε n (3.7) P {ϱ ( µ n, µ) ε n } ε n. (3.8) We show that the last obtaine subsequence (X n ) satisfies the conclusion of the theorem. In view of (2.4) an (3.4), X n an X are interchangeable in the statement of the theorem an thus it suffices to prove that if (X ) satisfies statements (A ), (B ), (C ) above then for any permutation (Y ) of (X ) we have (2.5). To verify this, note that by (2.4) an (3.6) we have { P A f (X i,..., X i l, µ A ) f (Z (A) i,..., Z (A) i l, µ A ) ε α } r q (3.9) ε α r q A Γ 2 where l = q p +, i,..., i l are ifferent integers > r an µ A is the probability measure corresponing to F A. (Note that we o not assume here i <... < i l ; the vectors (X i..., X i l ) an (Z (A) i,..., Z (A) i l ) are close to each other coorinatewise, i.e. for any orer of i,..., i l. Since the Z (A) j are i.i.., the istribution of the 8

9 vector (Z (A) i,..., Z (A) i l ) is permutation-invariant, proviing an explanation for the phenomenon escribe in Theorem 2.2.) Since (3.9) is vali for all A Γ 2 an µ A in (3.9) is ientical to µ r on A (see Lemma 6 of [5]), using (3.5), (3.9) an statement (B) at the beginning of the proof we get ϱ ( f (X i,..., X i l, µ r ), A f (µ A )P (A) ) 2ε α r q (3.0) where the sum is extene for all atoms A of σ{x r } an a r.v. in a Prohorov istance is meant as its istribution. Next we show that (3.0) remains vali, with the right han sie increase by r, if i,..., i l, l = q p +, are arbitrary ifferent positive integers (not necessarily > r ). Inee, remove from X i,..., X i l those whose inex is r an replace them with (ifferent) X j s with j > max(r, i,..., i l ). This means that we change f (X i,..., X i l, µ r ) at most at r locations an at each such position we replace an X µ by an X ν where µ r an ν > r. By (2.4), f changes at most by X ω µ X ν α =: W where the sum has r terms. Using (3.), (3.2) we get ( ) P ( W r ) P ( W ω /2 ) = P X µ X ν α ω /2 ( P X µ X ν ( /2 ω ) /α) ( 2r sup r j P X j 2 ω/(4α) ) r an thus the above changes increase the left han sie of (3.0) by at most r, i.e. ( ϱ f (X i,..., X i l, µ r ), ) f (µ A )P (A) 2ε α r q + r (3.) A for any ifferent positive integers i,..., i l, l = q p +. Changing µ r into µ will change f (X i,..., X i l, µ r ) on the left han sie of (3.) by at most ε r, except on a set of probability ε r (see (3.8) an (2.4)) an thus the left han sie of (3.) changes by at most ε r. Thus observing that the sum A f (µ A )P (A) in (3.) equals f ( µ r )P, we prove the following Proposition. Let (X ) be any permutation of (X ). Then ϱ ( f (Xp,..., Xq, µ), f ( µ r )P ) 3ε α r q + r. To complete the proof of our theorem it suffices to show that the Prohorov istance of any two of the istributions f ( µ r )P f ( µ)p G µ P (3.2) tens to zero as. To verify this observe first that (3.7), (3.8) an statement (A) at the beginning of the proof imply that the Prohorov istance of f ( µ r ) an 9

10 f ( µ) is ε α r q + ε r, except on a set with probability ε α r q + ε r an thus by statement (C) an (2.2) the Prohorov istance of the first two istributions in (3.2) is 2(ε α r q + ε r ) 4. On the other han, the valiity of f (µ) G µ for any µ S (which is a part of the efinition of a wea limit theorem) an P ( µ S) = imply ϱ(f ( µ), G µ ) 0 a.s. an thus there exists a numerical sequence δ 0 such that P {ϱ(f ( µ), G µ ) δ } δ ( =, 2,...). Thus by statement (C) above we get that the Prohorov istance of the secon an thir istribution in (3.2) is 2δ. This completes the proof of Theorem 2.2. Acnowlement. We woul lie to than two anonymous referees for their remars leaing to a substantial improvement of the presentation. References [] C. Aistleitner an I. Beres. On the central limit theorem for f(n x). Probab. Theory Rel. Fiels 46 (200), [2] C. Aistleitner, I. Beres an R. Tichy. On the law of the iterate logarithm for permute lacunary sequences. Proc. Stelov Inst. Math. 276 (202), [3] C. Aistleitner, I. Beres an R. Tichy. On permutations of lacunary series. RIMS Kôyûrou Bessatsu B34 (202), 25. [4] D. J. Alous. Limit theorems for subsequences of arbitrarily-epenent sequences of ranom variables, Z. Wahrscheinlicheitstheorie verw. Gebiete 40 (977), [5] I. Beres. An extension of the Komlós subsequence theorem. Acta Math. Hung. 55 (990) [6] I. Beres an E. Péter. Exchangeable ranom variables an the subsequence principle, Prob. Theory Rel. Fiels 73 (986), [7] I. Beres an H. P. Rosenthal. Almost exchangeable sequences of ranom variables, Z. Wahrscheinlicheitstheorie verw. Gebiete 70 (985), [8] S. D. Chatterji. A general strong law. Invent. Math / [9] S. D. Chatterji. A principle of subsequences in probability theory: The central limit theorem. Av. Math. 3 (974), [0] S. D. Chatterji. A subsequence principle in probability theory II. The law of the iterate logarithm. Invent. Math. 25 (974), pp Springer, 972. [] P. Erős. On trigonometric sums with gaps. Magyar Tu. Aa. Mat. Kut. Int. Közl. 7 (962),

11 [2] P. Erős an I.S. Gál. On the law of the iterate logarithm. Proc. Neerl. Aa. Wetensch. Ser A 58, 65-84, 955. [3] V. F. Gaposhin. Lacunary series an inepenent functions. Russian Math. Surveys 2 (966), [4] V. F. Gaposhin. Convergence an limit theorems for subsequences of ranom variables. (Russian) Teor. Verojatnost. i Primenen. 7 (972), [5] A. M. Garsia. Existence of almost everywhere convergent rearrangements for Fourier series of L 2 functions. Ann. of Math. 79 (964), [6] S. Guerre an Y. Raynau. On sequences with no almost symmetric subsequence. Texas Functional Analysis Seminar Longhorn Notes, Univ. of Texas pp Austin, 986. [7] A. N. Kolmogorov an D. Menshov. Sur la convergence es series e fonctions orthogonales. Math. Z. 26 (927), [8] J. Komlós. A generalization of a problem of Steinhaus. Acta Math. Aca. Sci. Hungar. 8, , (967) [9] J. Komlós. Every sequence converging to 0 wealy in L 2 contains an unconitional convergence sequence. Ar. Mat. 2 (974), [20] D. E. Menshov. Sur la convergence et la sommation es se ries e fonctions orthogonales. Bull. Soc. Math. France 60 (936), [2] E. Péter, An extension of the subsequence principle. Stuia Sci. Math. Hung. 36 (2000), [22] A. Rényi, On stable sequences of events. Sanhya Ser. A 25 (963), [23] P. Révész, On a problem of Steinhaus. Acta Math. Aca. Sci. Hung. 6 (965), [24] R. Salem an A. Zygmun. On lacunary trigonometric series, Proc. Nat. Aca. Sci. USA 33 (947), [25] R. Salem an A. Zygmun, La loi u logarithme itéré pour les séries trigonométriques lacunaires. Bull. Sci. Math. 74, , 950. [26] V. Strassen. The existence of probability measures with given marginals, Ann. Math. Statist. 36 (965), [27] S. Taahashi. On the law of the iterate logarithm for lacunary trigonometric series. Tohou Math. J. 24 (972),

The Kadec-Pe lczynski theorem in L p, 1 p < 2

The Kadec-Pe lczynski theorem in L p, 1 p < 2 The Kadec-Pe lczynski theorem in L p, 1 p < 2 I. Berkes and R. Tichy Abstract By a classical result of Kadec and Pe lczynski (1962), every normalized weakly null sequence in L p, p > 2 contains a subsequence

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

Logarithmic spurious regressions

Logarithmic spurious regressions Logarithmic spurious regressions Robert M. e Jong Michigan State University February 5, 22 Abstract Spurious regressions, i.e. regressions in which an integrate process is regresse on another integrate

More information

Topic 7: Convergence of Random Variables

Topic 7: Convergence of Random Variables Topic 7: Convergence of Ranom Variables Course 003, 2016 Page 0 The Inference Problem So far, our starting point has been a given probability space (S, F, P). We now look at how to generate information

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

Generalized Tractability for Multivariate Problems

Generalized Tractability for Multivariate Problems Generalize Tractability for Multivariate Problems Part II: Linear Tensor Prouct Problems, Linear Information, an Unrestricte Tractability Michael Gnewuch Department of Computer Science, University of Kiel,

More information

1. Aufgabenblatt zur Vorlesung Probability Theory

1. Aufgabenblatt zur Vorlesung Probability Theory 24.10.17 1. Aufgabenblatt zur Vorlesung By (Ω, A, P ) we always enote the unerlying probability space, unless state otherwise. 1. Let r > 0, an efine f(x) = 1 [0, [ (x) exp( r x), x R. a) Show that p f

More information

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM Teor Imov r. ta Matem. Statist. Theor. Probability an Math. Statist. Vip. 81, 1 No. 81, 1, Pages 147 158 S 94-911)816- Article electronically publishe on January, 11 UDC 519.1 A LIMIT THEOREM FOR RANDOM

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

On the law of the iterated logarithm for the discrepancy of lacunary sequences

On the law of the iterated logarithm for the discrepancy of lacunary sequences On the law of the iterated logarithm for the discrepancy of lacunary sequences Christoph Aistleitner Abstract A classical result of Philipp (1975) states that for any sequence (n k ) k 1 of integers satisfying

More information

Discrete Mathematics

Discrete Mathematics Discrete Mathematics 309 (009) 86 869 Contents lists available at ScienceDirect Discrete Mathematics journal homepage: wwwelseviercom/locate/isc Profile vectors in the lattice of subspaces Dániel Gerbner

More information

Sharp Thresholds. Zachary Hamaker. March 15, 2010

Sharp Thresholds. Zachary Hamaker. March 15, 2010 Sharp Threshols Zachary Hamaker March 15, 2010 Abstract The Kolmogorov Zero-One law states that for tail events on infinite-imensional probability spaces, the probability must be either zero or one. Behavior

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

The chromatic number of graph powers

The chromatic number of graph powers Combinatorics, Probability an Computing (19XX) 00, 000 000. c 19XX Cambrige University Press Printe in the Unite Kingom The chromatic number of graph powers N O G A A L O N 1 an B O J A N M O H A R 1 Department

More information

ON THE DISTANCE BETWEEN SMOOTH NUMBERS

ON THE DISTANCE BETWEEN SMOOTH NUMBERS #A25 INTEGERS (20) ON THE DISTANCE BETWEEN SMOOTH NUMBERS Jean-Marie De Koninc Département e mathématiques et e statistique, Université Laval, Québec, Québec, Canaa jm@mat.ulaval.ca Nicolas Doyon Département

More information

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

LECTURE NOTES ON DVORETZKY S THEOREM

LECTURE NOTES ON DVORETZKY S THEOREM LECTURE NOTES ON DVORETZKY S THEOREM STEVEN HEILMAN Abstract. We present the first half of the paper [S]. In particular, the results below, unless otherwise state, shoul be attribute to G. Schechtman.

More information

arxiv: v1 [math.mg] 10 Apr 2018

arxiv: v1 [math.mg] 10 Apr 2018 ON THE VOLUME BOUND IN THE DVORETZKY ROGERS LEMMA FERENC FODOR, MÁRTON NASZÓDI, AND TAMÁS ZARNÓCZ arxiv:1804.03444v1 [math.mg] 10 Apr 2018 Abstract. The classical Dvoretzky Rogers lemma provies a eterministic

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition

More information

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS ALINA BUCUR, CHANTAL DAVID, BROOKE FEIGON, MATILDE LALÍN 1 Introuction In this note, we stuy the fluctuations in the number

More information

An extension of Alexandrov s theorem on second derivatives of convex functions

An extension of Alexandrov s theorem on second derivatives of convex functions Avances in Mathematics 228 (211 2258 2267 www.elsevier.com/locate/aim An extension of Alexanrov s theorem on secon erivatives of convex functions Joseph H.G. Fu 1 Department of Mathematics, University

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

On the central limit theorem for f (n k x)

On the central limit theorem for f (n k x) Probab. Theory Relat. Fields (1) 146:67 89 DOI 1.17/s44-8-19-6 On the central limit theorem for f (n k x) Christoph Aistleitner István Berkes Received: 9 May 8 / Revised: 3 September 8 / Published online:

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

Interconnected Systems of Fliess Operators

Interconnected Systems of Fliess Operators Interconnecte Systems of Fliess Operators W. Steven Gray Yaqin Li Department of Electrical an Computer Engineering Ol Dominion University Norfolk, Virginia 23529 USA Abstract Given two analytic nonlinear

More information

Introduction to Markov Processes

Introduction to Markov Processes Introuction to Markov Processes Connexions moule m44014 Zzis law Gustav) Meglicki, Jr Office of the VP for Information Technology Iniana University RCS: Section-2.tex,v 1.24 2012/12/21 18:03:08 gustav

More information

On colour-blind distinguishing colour pallets in regular graphs

On colour-blind distinguishing colour pallets in regular graphs J Comb Optim (2014 28:348 357 DOI 10.1007/s10878-012-9556-x On colour-blin istinguishing colour pallets in regular graphs Jakub Przybyło Publishe online: 25 October 2012 The Author(s 2012. This article

More information

On the enumeration of partitions with summands in arithmetic progression

On the enumeration of partitions with summands in arithmetic progression AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Some Examples. Uniform motion. Poisson processes on the real line

Some Examples. Uniform motion. Poisson processes on the real line Some Examples Our immeiate goal is to see some examples of Lévy processes, an/or infinitely-ivisible laws on. Uniform motion Choose an fix a nonranom an efine X := for all (1) Then, {X } is a [nonranom]

More information

Conservation Laws. Chapter Conservation of Energy

Conservation Laws. Chapter Conservation of Energy 20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

Iterated Point-Line Configurations Grow Doubly-Exponentially

Iterated Point-Line Configurations Grow Doubly-Exponentially Iterate Point-Line Configurations Grow Doubly-Exponentially Joshua Cooper an Mark Walters July 9, 008 Abstract Begin with a set of four points in the real plane in general position. A to this collection

More information

AN IMPROVED MENSHOV-RADEMACHER THEOREM

AN IMPROVED MENSHOV-RADEMACHER THEOREM PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 124, Number 3, March 1996 AN IMPROVED MENSHOV-RADEMACHER THEOREM FERENC MÓRICZ AND KÁROLY TANDORI (Communicated by J. Marshall Ash) Abstract. We

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

arxiv: v4 [math.pr] 27 Jul 2016

arxiv: v4 [math.pr] 27 Jul 2016 The Asymptotic Distribution of the Determinant of a Ranom Correlation Matrix arxiv:309768v4 mathpr] 7 Jul 06 AM Hanea a, & GF Nane b a Centre of xcellence for Biosecurity Risk Analysis, University of Melbourne,

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

Survival exponents for fractional Brownian motion with multivariate time

Survival exponents for fractional Brownian motion with multivariate time Survival exponents for fractional Brownian motion with multivariate time G Molchan Institute of Earthquae Preiction heory an Mathematical Geophysics Russian Acaemy of Science 84/3 Profsoyuznaya st 7997

More information

A Weak First Digit Law for a Class of Sequences

A Weak First Digit Law for a Class of Sequences International Mathematical Forum, Vol. 11, 2016, no. 15, 67-702 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1288/imf.2016.6562 A Weak First Digit Law for a Class of Sequences M. A. Nyblom School of

More information

Lecture 2: Correlated Topic Model

Lecture 2: Correlated Topic Model Probabilistic Moels for Unsupervise Learning Spring 203 Lecture 2: Correlate Topic Moel Inference for Correlate Topic Moel Yuan Yuan First of all, let us make some claims about the parameters an variables

More information

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

WUCHEN LI AND STANLEY OSHER

WUCHEN LI AND STANLEY OSHER CONSTRAINED DYNAMICAL OPTIMAL TRANSPORT AND ITS LAGRANGIAN FORMULATION WUCHEN LI AND STANLEY OSHER Abstract. We propose ynamical optimal transport (OT) problems constraine in a parameterize probability

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

LEGENDRE TYPE FORMULA FOR PRIMES GENERATED BY QUADRATIC POLYNOMIALS

LEGENDRE TYPE FORMULA FOR PRIMES GENERATED BY QUADRATIC POLYNOMIALS Ann. Sci. Math. Québec 33 (2009), no 2, 115 123 LEGENDRE TYPE FORMULA FOR PRIMES GENERATED BY QUADRATIC POLYNOMIALS TAKASHI AGOH Deicate to Paulo Ribenboim on the occasion of his 80th birthay. RÉSUMÉ.

More information

arxiv: v1 [math.co] 15 Sep 2015

arxiv: v1 [math.co] 15 Sep 2015 Circular coloring of signe graphs Yingli Kang, Eckhar Steffen arxiv:1509.04488v1 [math.co] 15 Sep 015 Abstract Let k, ( k) be two positive integers. We generalize the well stuie notions of (k, )-colorings

More information

Conservation laws a simple application to the telegraph equation

Conservation laws a simple application to the telegraph equation J Comput Electron 2008 7: 47 51 DOI 10.1007/s10825-008-0250-2 Conservation laws a simple application to the telegraph equation Uwe Norbrock Reinhol Kienzler Publishe online: 1 May 2008 Springer Scienceusiness

More information

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH English NUMERICAL MATHEMATICS Vol14, No1 Series A Journal of Chinese Universities Feb 2005 TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH He Ming( Λ) Michael K Ng(Ξ ) Abstract We

More information

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy, NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which

More information

Abstract A nonlinear partial differential equation of the following form is considered:

Abstract A nonlinear partial differential equation of the following form is considered: M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent

More information

A FURTHER REFINEMENT OF MORDELL S BOUND ON EXPONENTIAL SUMS

A FURTHER REFINEMENT OF MORDELL S BOUND ON EXPONENTIAL SUMS A FURTHER REFINEMENT OF MORDELL S BOUND ON EXPONENTIAL SUMS TODD COCHRANE, JEREMY COFFELT, AND CHRISTOPHER PINNER 1. Introuction For a prime p, integer Laurent polynomial (1.1) f(x) = a 1 x k 1 + + a r

More information

1. A remark to the law of the iterated logarithm. Studia Sci. Math. Hung. 7 (1972)

1. A remark to the law of the iterated logarithm. Studia Sci. Math. Hung. 7 (1972) 1 PUBLICATION LIST OF ISTVÁN BERKES 1. A remark to the law of the iterated logarithm. Studia Sci. Math. Hung. 7 (1972) 189-197. 2. Functional limit theorems for lacunary trigonometric and Walsh series.

More information

REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE. 1. Introduction We look at the problem of reversibility for operators of the form

REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE. 1. Introduction We look at the problem of reversibility for operators of the form REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE OMAR RIVASPLATA, JAN RYCHTÁŘ, AND BYRON SCHMULAND Abstract. Why is the rift coefficient b associate with a reversible iffusion on R given by a graient?

More information

Lecture 1: Review of Basic Asymptotic Theory

Lecture 1: Review of Basic Asymptotic Theory Lecture 1: Instructor: Department of Economics Stanfor University Prepare by Wenbo Zhou, Renmin University Basic Probability Theory Takeshi Amemiya, Avance Econometrics, 1985, Harvar University Press.

More information

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945

More information

MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX

MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX J. WILLIAM HELTON, JEAN B. LASSERRE, AND MIHAI PUTINAR Abstract. We investigate an iscuss when the inverse of a multivariate truncate moment matrix

More information

arxiv:math/ v1 [math.pr] 19 Apr 2001

arxiv:math/ v1 [math.pr] 19 Apr 2001 Conitional Expectation as Quantile Derivative arxiv:math/00490v math.pr 9 Apr 200 Dirk Tasche November 3, 2000 Abstract For a linear combination u j X j of ranom variables, we are intereste in the partial

More information

arxiv: v1 [math.co] 13 Dec 2017

arxiv: v1 [math.co] 13 Dec 2017 The List Linear Arboricity of Graphs arxiv:7.05006v [math.co] 3 Dec 07 Ringi Kim Department of Mathematical Sciences KAIST Daejeon South Korea 344 an Luke Postle Department of Combinatorics an Optimization

More information

SOME RESULTS ASSOCIATED WITH FRACTIONAL CALCULUS OPERATORS INVOLVING APPELL HYPERGEOMETRIC FUNCTION

SOME RESULTS ASSOCIATED WITH FRACTIONAL CALCULUS OPERATORS INVOLVING APPELL HYPERGEOMETRIC FUNCTION Volume 29), Issue, Article 4, 7 pp. SOME RESULTS ASSOCIATED WITH FRACTIONAL CALCULUS OPERATORS INVOLVING APPELL HYPERGEOMETRIC FUNCTION R. K. RAINA / GANPATI VIHAR, OPPOSITE SECTOR 5 UDAIPUR 332, RAJASTHAN,

More information

Quantum mechanical approaches to the virial

Quantum mechanical approaches to the virial Quantum mechanical approaches to the virial S.LeBohec Department of Physics an Astronomy, University of Utah, Salt Lae City, UT 84112, USA Date: June 30 th 2015 In this note, we approach the virial from

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

REAL ANALYSIS I HOMEWORK 5

REAL ANALYSIS I HOMEWORK 5 REAL ANALYSIS I HOMEWORK 5 CİHAN BAHRAN The questions are from Stein an Shakarchi s text, Chapter 3. 1. Suppose ϕ is an integrable function on R with R ϕ(x)x = 1. Let K δ(x) = δ ϕ(x/δ), δ > 0. (a) Prove

More information

Lyapunov Functions. V. J. Venkataramanan and Xiaojun Lin. Center for Wireless Systems and Applications. School of Electrical and Computer Engineering,

Lyapunov Functions. V. J. Venkataramanan and Xiaojun Lin. Center for Wireless Systems and Applications. School of Electrical and Computer Engineering, On the Queue-Overflow Probability of Wireless Systems : A New Approach Combining Large Deviations with Lyapunov Functions V. J. Venkataramanan an Xiaojun Lin Center for Wireless Systems an Applications

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

arxiv: v2 [math.pr] 27 Nov 2018

arxiv: v2 [math.pr] 27 Nov 2018 Range an spee of rotor wals on trees arxiv:15.57v [math.pr] 7 Nov 1 Wilfrie Huss an Ecaterina Sava-Huss November, 1 Abstract We prove a law of large numbers for the range of rotor wals with ranom initial

More information

Tractability results for weighted Banach spaces of smooth functions

Tractability results for weighted Banach spaces of smooth functions Tractability results for weighte Banach spaces of smooth functions Markus Weimar Mathematisches Institut, Universität Jena Ernst-Abbe-Platz 2, 07740 Jena, Germany email: markus.weimar@uni-jena.e March

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

Consistency and asymptotic normality

Consistency and asymptotic normality Consistency an asymtotic normality Class notes for Econ 842 Robert e Jong March 2006 1 Stochastic convergence The asymtotic theory of minimization estimators relies on various theorems from mathematical

More information

A simple model for the small-strain behaviour of soils

A simple model for the small-strain behaviour of soils A simple moel for the small-strain behaviour of soils José Jorge Naer Department of Structural an Geotechnical ngineering, Polytechnic School, University of São Paulo 05508-900, São Paulo, Brazil, e-mail:

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Noether s theorem applied to classical electrodynamics

Noether s theorem applied to classical electrodynamics Noether s theorem applie to classical electroynamics Thomas B. Mieling Faculty of Physics, University of ienna Boltzmanngasse 5, 090 ienna, Austria (Date: November 8, 207) The consequences of gauge invariance

More information

arxiv: v1 [math.co] 31 Mar 2008

arxiv: v1 [math.co] 31 Mar 2008 On the maximum size of a (k,l)-sum-free subset of an abelian group arxiv:080386v1 [mathco] 31 Mar 2008 Béla Bajnok Department of Mathematics, Gettysburg College Gettysburg, PA 17325-186 USA E-mail: bbajnok@gettysburgeu

More information

Pseudo-Free Families of Finite Computational Elementary Abelian p-groups

Pseudo-Free Families of Finite Computational Elementary Abelian p-groups Pseuo-Free Families of Finite Computational Elementary Abelian p-groups Mikhail Anokhin Information Security Institute, Lomonosov University, Moscow, Russia anokhin@mccme.ru Abstract We initiate the stuy

More information

Acute sets in Euclidean spaces

Acute sets in Euclidean spaces Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of

More information

ON TAUBERIAN CONDITIONS FOR (C, 1) SUMMABILITY OF INTEGRALS

ON TAUBERIAN CONDITIONS FOR (C, 1) SUMMABILITY OF INTEGRALS REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 54, No. 2, 213, Pages 59 65 Publishe online: December 8, 213 ON TAUBERIAN CONDITIONS FOR C, 1 SUMMABILITY OF INTEGRALS Abstract. We investigate some Tauberian

More information

Gradient flow of the Chapman-Rubinstein-Schatzman model for signed vortices

Gradient flow of the Chapman-Rubinstein-Schatzman model for signed vortices Graient flow of the Chapman-Rubinstein-Schatzman moel for signe vortices Luigi Ambrosio, Eoaro Mainini an Sylvia Serfaty Deicate to the memory of Michelle Schatzman (1949-2010) Abstract We continue the

More information

Robustness and Perturbations of Minimal Bases

Robustness and Perturbations of Minimal Bases Robustness an Perturbations of Minimal Bases Paul Van Dooren an Froilán M Dopico December 9, 2016 Abstract Polynomial minimal bases of rational vector subspaces are a classical concept that plays an important

More information

Monotonicity for excited random walk in high dimensions

Monotonicity for excited random walk in high dimensions Monotonicity for excite ranom walk in high imensions Remco van er Hofsta Mark Holmes March, 2009 Abstract We prove that the rift θ, β) for excite ranom walk in imension is monotone in the excitement parameter

More information

Continuity equations and ODE flows with non-smooth velocity

Continuity equations and ODE flows with non-smooth velocity Continuity equations an ODE flows with non-smooth velocity Luigi Ambrosio an Gianluca Crippa Einburgh, April 15-16, 213 Contents 1 Introuction 1 2 Transport equation an continuity equation within the Cauchy-Lipschitz

More information

WAVELET-BASED ESTIMATORS OF THE INTEGRATED SQUARED DENSITY DERIVATIVES FOR MIXING SEQUENCES

WAVELET-BASED ESTIMATORS OF THE INTEGRATED SQUARED DENSITY DERIVATIVES FOR MIXING SEQUENCES Pa. J. Statist. 009 Vol. 5(3), 3-350 WAVELET-BASED ESTIMATORS OF THE INTEGRATED SQUARED DENSITY DERIVATIVES FOR MIXING SEQUENCES N. Hosseinioun, H. Doosti an H.A. Nirouan 3 Departent of Statistics, School

More information

Bisecting Sparse Random Graphs

Bisecting Sparse Random Graphs Bisecting Sparse Ranom Graphs Malwina J. Luczak,, Colin McDiarmi Mathematical Institute, University of Oxfor, Oxfor OX 3LB, Unite Kingom; e-mail: luczak@maths.ox.ac.uk Department of Statistics, University

More information

3 The variational formulation of elliptic PDEs

3 The variational formulation of elliptic PDEs Chapter 3 The variational formulation of elliptic PDEs We now begin the theoretical stuy of elliptic partial ifferential equations an bounary value problems. We will focus on one approach, which is calle

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

Ramsey numbers of some bipartite graphs versus complete graphs

Ramsey numbers of some bipartite graphs versus complete graphs Ramsey numbers of some bipartite graphs versus complete graphs Tao Jiang, Michael Salerno Miami University, Oxfor, OH 45056, USA Abstract. The Ramsey number r(h, K n ) is the smallest positive integer

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

Exponential asymptotic property of a parallel repairable system with warm standby under common-cause failure

Exponential asymptotic property of a parallel repairable system with warm standby under common-cause failure J. Math. Anal. Appl. 341 (28) 457 466 www.elsevier.com/locate/jmaa Exponential asymptotic property of a parallel repairable system with warm stanby uner common-cause failure Zifei Shen, Xiaoxiao Hu, Weifeng

More information

On the Cauchy Problem for Von Neumann-Landau Wave Equation

On the Cauchy Problem for Von Neumann-Landau Wave Equation Journal of Applie Mathematics an Physics 4 4-3 Publishe Online December 4 in SciRes http://wwwscirporg/journal/jamp http://xoiorg/436/jamp4343 On the Cauchy Problem for Von Neumann-anau Wave Equation Chuangye

More information

The central limit theorem for subsequences in probabilistic number theory

The central limit theorem for subsequences in probabilistic number theory The central limit theorem for subsequences in probabilistic number theory Christoph Aistleitner, Christian Elsholtz Abstract Let ( ) k be an increasing sequence of positive integers, and let f(x) be a

More information

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information