Prediction on a Graph with a Perceptron
|
|
- Joella Wilkinson
- 6 years ago
- Views:
Transcription
1 Predition on a Graph with a Pereptron Mark Herbster, Massimiliano Pontil Department of Computer Siene University College London Gower Street, London WC1E 6BT, England, UK {m.herbster, m.pontil}@s.ul.a.uk Abstrat We study the problem of online predition of a noisy labeling of a graph with the pereptron. We address both label noise and onept noise. Graph learning is framed as an instane of predition on a finite set. To treat label noise we show that the hinge loss bounds derived by Gentile [1] for online pereptron learning an be transformed to relative mistake bounds with an optimal leading onstant when applied to predition on a finite set. These bounds depend ruially on the norm of the learned onept. Often the norm of a onept an vary dramatially with only small perturbations in a labeling. We analyze a simple transformation that stabilizes the norm under perturbations. We derive an upper bound that depends only on natural properties of the graph the graph diameter and the ut size of a partitioning of the graph whih are only indiretly dependent on the size of the graph. The impossibility of suh bounds for the graph geodesi nearest neighbors algorithm will be demonstrated. 1 Introdution We study the problem of robust online learning over a graph. Consider the following game for prediting the labeling of a graph. Nature presents a vertex v i1 ; the learner predits the label of the vertex ŷ 1 { 1, 1}; nature presents a label y 1 ; nature presents a vertex v i2 ; the learner predits ŷ 2 ; and so forth. The learner s goal is minimize the total number of mistakes ( {t : ŷ t y t } ). If nature is adversarial, the learner will always mispredit; but if nature is regular or simple, there is hope that a learner may make only a few mispreditions. Thus, a methodologial goal is to give learners whose total mispreditions an be bounded relative to the omplexity of nature s labeling. In this paper, we onsider the ut size as a measure of the omplexity of a graph s labeling, where the size of the ut is the number of edges between disagreeing labels. We will give bounds whih depend on the ut size and the diameter of the graph and thus do not diretly depend on the size of the graph. The problem of learning a labeling of a graph is a natural problem in the online learning setting, as well as a foundational tehnique for a variety of semisupervised learning methods [2, 3, 4, 5, 6]. For example, in the online setting, onsider a system whih serves advertisements on web pages. The web pages may be identified with the verties of a graph and the edges as links between pages. The online predition problem is then that, at a given time t the system may reeive a request to serve an advertisement on a partiular web page. For simpliity, we assume that there are two alternatives to be served: either advertisement A or advertisement B. The system then interprets the feedbak as the label and then may use this information in responding to the next request to predit an advertisement for a requested web page. 1.1 Related work There is a welldeveloped literature regarding learning on the graph. The early work of Blum and Chawla [2] presented an algorithm whih expliitly finds minuts of the label set. Bounds have been
2 Input: {(v it, y t)} l t=1 V M { 1,1}. Initialization: w 1 = 0; M A =. for t = 1,..., l do Predit: reeive v it ŷ t = sign(e i t w t) Update: reeive y t if ŷ t = y t then w t1 = w t else w t1 = w t y tv it M A = M A {t} end Figure 1: Pereptron on set V M. Figure 2: Barbell Figure 3:Barbell with onept noise Figure 4: Flower Figure 5: Otopus proven previously with smooth loss funtions [6, 7] in a bath setting. Kernels on graph labelings were introdued in [3, 5]. This urrent work builds upon our work in [8]. There it was shown that, given a fixed labeling of a graph, the number of mistakes made by an algorithm similar to the kernel pereptron [9] with a kernel that was the pseudoinverse of the graph Laplaian, ould be bounded by the quantity [8, Theorems 3.2, 4.1, and 4.2] 4Φ G (u)d G bal(u). (1) Here u { 1, 1} n is a binary vetor defining the labeling of the graph, Φ G (u) is the ut size 1 defined as Φ G (u) := {(i, j) E(G) : u i u j }, that is, the number of edges between positive and negative labels, D G is the diameter of the graph and bal(u) := ( 1 1 n u i ) 2 measures the label balane. This bound is interesting in that the mistakes of the algorithm ould be bounded in terms of simple properties of a labeled graph. However, there are a variety of shortomings in this result. First, we observe that the bound above assumed a fixed labeling of the graph. In pratie, the online data sequene ould ontain multiple labels for a single vertex; this is the problem of label noise. Seond, for an unbalaned set of labels the bound is vauous, for example, if u = {1, 1,..., 1, 1} IR n then bal(u) = n 2. Third, onsider the prototypial easy instane for the algorithm of two dense lusters onneted by a few edges, for instane, two mliques onneted by a single edge (a barbell graph, see Figure 2). If eah lique is labeled with distint labels then we have that 4Φ G (u)d G bal(u) = = 12, whih is independent of m. Now suppose that, say, the first lique ontains one vertex whih is labeled as the seond lique (see Figure 3). Previously Φ G (u) = 1, but now Φ G (u) = m and the bound is vauous. This is the problem of onept noise; in this example, a Θ(1) perturbation of labeling inreases the bound multipliatively by Θ(m). 1.2 Overview A first aim of this paper is to improve upon the bounds in [8], partiularly, to address the three problems of label balane, label noise, and onept noise as disussed above. For this purpose, we apply the wellknown kernel pereptron [9] to the problem of online learning on the graph. We disuss the bakground material for this problem in setion 2, where we also show that the bounds of [1] an be speialized to relative mistake bounds when applied to, for example, predition on the graph. A seond important aim of this paper is to interpret the mistake bounds by an explanation in terms of high level graph properties. Hene, in setion 3, we refine a diameter based bound of [8, Theorem 4.2] to a sharper bound based on the resistane distane [10] on a weighted graph; whih we then losely math with a lower bound. In setion 4, we introdue a kernel whih is a simple augmentation of the pseudoinverse of the graph Laplaian and then prove a theorem on the performane of the pereptron with this kernel whih solves the three problems above. We onlude in setion 5, with a disussion omparing the mistake bounds for predition on the graph with the halving algorithm [11] and the knearest neighbors algorithm. 2 Preliminaries In this setion, we desribe our setup for Hilbert spaes on finite sets and its speifiation to the graph ase. We then reall a result of Gentile [1] on predition with the pereptron and disuss a speial ase in whih relative 0 1 loss (mistake) bounds are obtainable. 1 Later in the paper we extend the definition of ut size to weighted graphs.
3 2.1 Hilbert spaes of funtions defined on a finite set We denote matries by apital bold letters and vetors by small bold ase letters. So M denotes the n n matrix (M ij ) n i,j=1 and w the ndimensional vetor (w i) n i=1. The identity matrix is denoted by I. We also let 0 and 1 be the ndimensional vetors all of whose omponents equal to zero and one respetively, and e i the ith oordinate vetor of IR n. Let IN be the set of natural numbers and IN l := {1,..., l}. We denote a generi Hilbert spae with H. We identify V := IN n as the indies of a set of n objets, e.g. the verties of a graph. A vetor w IR n an alternatively be seen as a funtion f : V IR suh that f(i) = w i, i V. However, for simpliity we will use the notation w to denote both a vetor in IR n or the above funtion. A symmetri positive semidefinite matrix M indues a semiinner produt on IR n whih is defined as u, w M := u Mw, where denotes transposition. The reproduing kernel [12] assoiated with the above semiinner produt is K = M, where denotes pseudoinverse. We also define the oordinate spanning set V M := {v i := M e i : i = 1,..., n} (2) and let H(M) := span(v M ). The restrition of the semiinner produt, M to H(M) is an inner produt on H(M). The set V M ats as oordinates for H(M), that is, if w H(M) we have w i = e i M Mw = v i Mw = v i, w M, (3) although the vetors {v 1,..., v n } are not neessarily normalized and are linearly independent only if M is positive definite. We note that equation (3) is simply the reproduing kernel property [12] for kernel M. When V indexes the verties of an undireted graph G, a natural norm to use is that indued by the graph Laplaian. We explain this in detail now. Let A be the n n symmetri weight matrix of the graph suh that A ij 0, and define the edge set E(G) := {(i, j) : 0 < A ij, i < j}. The distane matrix assoiated with G is the perelement inverse of the weight matrix, that is, ij = 1 A ij ( may have as a matrix element). The graph Laplaian G is the n n matrix defined as G := D A where D = diag(d 1,..., d n ) and d i is the weighted degree of vertex i, d i = n j=1 A ij. The Laplaian is positive semidefinite and indues the seminorm w 2 G := w Gw = A ij (w i w j ) 2. (4) (i,j) E(G) When the graph is onneted, it follows from equation (4) that the null spae of G is spanned by the onstant vetor 1 only. In this paper, we always assume that the graph G is onneted. Where it is not ambiguous, we use the notation G to denote both the graph G and the graph Laplaian. 2.2 Online predition of funtions on a finite set with the pereptron Gentile [1] bounded the performane of the pereptron algorithm on nonseparable data with the linear hinge loss. Here, we apply his result to study the problem of predition on a finite set with the pereptron (see Figure 1). In this ase, the inputs are the oordinates in the set V M H(M) defined above. We additionally assume that matrix M is positive definite (not just positive semidefinite as in the previous subsetion). This assumption, along with the fat that the inputs are oordinates, enables us to upper bound the hinge loss and hene we may give a relative mistake bound in terms of the omplete set of base lassifiers { 1, 1} n. Theorem 2.1. Let M be a symmetri positive definite matrix. If {(v it, y t )} l t=1 V M { 1, 1} is a sequene of examples, M A denotes the set of trials in whih the pereptron algorithm predited inorretly and X = max t MA v it M, then the umulative number of mistakes M A of the algorithm is bounded by M A 2 M A M u u 2 M X2 2 2 M A M u u 2 M X2 u 4 M X4 4 for all u { 1, 1} n, where M u = {t IN l : u it y t }. In partiular, if M u = 0 then M A u 2 M X2. (5)
4 Proof. This bound follows diretly from [1, Theorem 8] with p = 2, γ = 1, and w 1 = 0. Sine M is assumed to be symmetri positive definite, it follows that { 1, 1} n H(M). Thus, the hinge loss L u,t := max(0, 1 y t u, v it M ) of any lassifier u { 1, 1} n with any example (v it, y t ) is either 0 or 2, sine u, v it M = 1 by equation (3). This allows us to bound the hinge loss term of [1, Theorem 8] diretly with mistakes. We emphasize that our hypothesis on M does not imply linear separability sine multiple instanes of an input vetor in the training sequene may have distint target labels. Moreover, we note that, for deterministi predition the onstant 2 in the first term of the right hand side of equation (5) is optimal for an online algorithm as a mistake may be fored on every trial. 3 Interpretation of the spae H(G) The bound for predition on a finite set in equation (5) involves two quantities, namely the squared norm of a lassifier u { 1, 1} n and the maximum of the squared norms of the oordinates v V M. In the ase of predition on the graph, reall from equation (4) that u 2 G := Gu = u (i,j) E(G) A ij(u i u j ) 2. Therefore, we may identify this seminorm with the weighted ut size Φ G (u) := 1 4 u 2 G (6) of the labeling indued when u { 1, 1} n. In partiular, with boolean weighted edges (A ij {0, 1}) the ut simply ounts the number of edges spanning disagreeing labels. The norm v w G is a metri distane for v, w span(v G ) however, surprisingly, the square of the norm v p v q 2 G when restrited to graph oordinates v p, v q V G is also a metri known as the resistane distane [10], r G (p, q) := (e p e q ) G (e p e q ) = v p v q 2 G. (7) It is interesting to note that the resistane distane between vertex p and vertex q is the effetive resistane between verties p and q, where the graph is the iruit and edge (i, j) is a resistor with the resistane ij = A 1 ij. As we shall see, our bounds in setion 4 depend on v p 2 G = v p 0 2 G. Formally, this is not an effetive resistane between vertex p and another vertex 0. The vetor 0, informally however, is P v V v G the enter of the graph as 0 = V G, sine 1 is in the null spae of H(G). In the following, we further haraterize v p 2 G. First, we observe qualitatively that the more interonneted the graph the smaller the term v p 2 G (Corollary 3.1). Seond, in Theorem 3.2 we quantitatively upper bound v p 2 G by the average (over q) of the effetive resistane between vertex p and eah vertex q in the graph (inluding q = p), whih in turn may be upper bounded by the eentriity of p. We proeed with the following useful lemma and theorem, as a basis for our later results. Lemma 3.1. Let x H then x 2 = min w H { w 2 : w, x = 1 }. The proof is straightforward and we do not elaborate on the details. Theorem 3.1. If M and M are symmetri positive semidefinite matries with span(v M ) = span(v M ) and, for every w span(v M ), w 2 M w 2 M then n 2 a i v i n a i v i 2, M M i=1 where v i V M, v i V M and a IRn. Proof. Let x = n i=1 a iv i and x = n i=1 a iv i then 2 x 2 M = x x 2 x 2 M M x 2 x 2 M M x 2 = x 2 M, M M x where the first inequality follows sine x, = 1, hene x 2 M x M is a feasible solution to x 2 M the minimization problem in the right hand side of Lemma 3.1. While the seond one follows immediately from the assumption that w 2 M w 2 M. i=1
5 As a orollary to the above theorem we have the following when M is a graph Laplaian. Corollary 3.1. Given onneted graphs G and G with distane matries and suh that ij ij then for all p, q V, we have that v p 2 G v p 2 G and r G (p, q) r G (p, q). The first inequality in the above orollary demonstrates that v p 2 G is noninreasing in a graph that is stritly more onneted. The seond inequality is the wellknown Rayleigh s monotoniity law whih states that if any resistane in a iruit is dereased then the effetive resistane between any two points annot inrease. We define the geodesi distane between verties p, q V to be d G (p, q) := min P (p, q) where the minimum is taken with respet to all paths P(p, q) from p to q, with the path length defined as P(p, q) := (i,j) E(P(p,q)) ij. The eentriity d G (p) of a vertex p V is the geodesi distane on the graph between p and the furthest vertex on the graph to p, that is, d G (p) = max q V d G (p, q) D G, and D G is the (geodesi) diameter of the graph, D G := max p V d G (p). A graph G is onneted when D G <. A tree is an nvertex onneted graph with n 1 edges. The following lemma, a well known result (see e.g. [10]), establishes that the resistane distane an be be equated with the geodesi distane when the graph is a tree. Lemma 3.2. If the graph T is a tree with graph Laplaian T then r T (p, q) = d T (p, q). The next theorem provides a quantitative relationship between v p 2 G and two measures of the onnetivity of vertex p, namely its eentriity and the mean of the effetive resistanes between vertex p and eah vertex on the graph. Theorem 3.2. If G is a onneted graph then v p 2 G 1 n r G (p, q) d G (p). (8) n q=1 Proof. Reall that r G (p, q) = v p v q 2 G (see equation (7)) and use n q=1 v q = 0 to obtain that 1 n n q=1 v p v q 2 G = v p Gv p 1 n n q=1 v q Gv q whih implies the left inequality in (8). Next, by Corollary 3.1, if T is the Laplaian of a tree T G then r G (p, q) r T (p, q) for p, q V. Therefore, from Lemma 3.2 we onlude that r G (p, q) d T (p, q). Moreover, sine T G an be any tree, we have that r G (p, q) min T d T (p, q) where the minimum is over all trees T G. Sine the geodesi path from p to q is neessarily ontained in some tree T G it follows that min T d T (p, q) = d G (p, q) and, so, r G (p, q) d G (p, q). Now the theorem follows by maximizing d G (p, q) over q and the definition of d G (p). We identify the resistane diameter of a graph G as R G := max p,q V r G (p, q); thus, from the previous theorem, we may also onlude that max v p 2 p V G R G D G. (9) We omplete this setion by showing that there exists a family of graphs for whih the above inequality is nearly tight. Speifially, we onsider the flower graph (see Figure 4) obtained by onneting the first vertex of a hain with p 1 verties to the root vertex of an mary tree of depth one. We index the verties of this graph so that verties 1 to p orrespond to stem verties and verties p 1 to p m to petals. Clearly, this graph has diameter equal to p, hene our upper bound above establishes that v 1 2 G p. We now argue that as m grows this bound is almost tight. From Lemma 3.1 we have that v 1 2 G = min { w H(G) w 2 G : w, v 1 = 1 }. We note that by symmetry, the solution ŵ = (ŵ i : i IN pm ) to the problem above satisfies ŵ i = z if i p 1 sine{ ŵ must take the same value on the petal verties. Consequently, it follows that v 1 2 G = min m(z w p ) 2 p 1 i=1 (w i w i1 ) 2 p : w 1 = 1, i=1 w i mz = 0}. We upper bound this minimum by hoosing w i = p i p 1 for 1 i p. Thus, w 1 = 1 as it is required, w p = 0 and we ompute z by the onstraint set of the above minimization problem as z = p 2m. A diret omputation gives v 1 2 G 1 (p 1) p2 4m from whih using a first order Taylor expansion it follows that v 1 2 G (p 1) (p 1)2 p 2 4m. Therefore, as m the upper bound on v 1 2 G (equation (8)) for the flower graph is mathed by a lower bound with a gap of 1.
6 4 Predition on the graph We define the following symmetri positive definite graph kernel, K b := G b11 I, (0 < b, 0 ), (10) where G b = (K b ) 1 is the matrix of the assoiated Hilbert spae H(G b ). In Lemma 4.1 below we prove the needed properties of H(G b ) as a neessary step for the bound in Theorem 4.2. As we shall see, these properties moderate the onsequenes of label imbalane and onept noise. To prove Lemma 4.1, we use the following theorem whih is a speial ase of [12, Thm I, I.6]. Theorem 4.1. If M 1 and M 2 are n n symmetri positive semidefinite matries, and we set M := (M 1 M 2 ) then w 2 M = inf{ w 1 2 M 1 w 2 2 M 2 : w i H(M i ), w 1 w 2 = w} for every w H(M). Next, we define β u [0, 1] as a measure of the balane of a labeling u { 1, 1} n as β u := ( 1 n n i=1 u i) 2. Note that for a perfetly balaned labeling β u = 0, while β u = 1 for a perfetly unbalaned one. Lemma 4.1. Given a vertex p with assoiated oordinates v p V G and v p V G b we have that v p 2 = v G b p 2 G b. (11) Moreover, if u, u { 1, 1} n and where k := {i : u i u i} we have that u 2 G b u 2 G β u b 4k. (12) Proof. To prove equation (11) we reall equation (3) and note that v p 2 G b = v p, v p b1e p G b = v p, v p G b v p, b1e p G b = v p 2 G b. To prove inequality (12) we proeed in two steps. First, we show that u 2 G b 0 = u 2 G β u b. (13) Indeed, we an uniquely deompose u as the sum of a vetor in H(G) and one in H( 11 n 2 b ) as u = (u 1 1 n n i=1 u i) 1 1 n n i=1 u i. Therefore, by Theorem 4.1 we onlude that u 2 = G b 0 u β u 1 2 G β u 1 2 = u 2 11 G βu b, where u β u 1 2 G = u 2 G sine 1 H (G). n 2 b Seond, we show, for any symmetri positive definite matrix M, u, u { 1, 1} n and > 0, that u 2 M u 2 M 4k, (14) where M := (M 1 I) 1 and k := {i : u i u i}. To this end, we deompose u as a sum of two elements of H(M) and H( 1 I) as u = u (u u) and observe that u u 2 1 I = 4k. By Theorem 4.1 it then follows that u 2 M u 2 M u u 2 1 I = u 2 M 4k. Now inequality (12) follows by ombining equations (13) and (14) with M = G b 0. We an now state our relative mistake bound for online predition on the graph. Theorem 4.2. Let G be a onneted graph. If {(v it, y t )} l t=1 V G b { 1, 1} is a sequene of examples and M A denotes the set of trials in whih the pereptron algorithm predited inorretly, then the umulative number of mistakes M A of the algorithm is bounded by M A 2 M A M u Z 2 2 M A M u Z Z2 4, (15) for all u,u { 1, 1} n, where k = {i:u i u i}, β u =( 1 n n i=1 u i )2, M u ={t IN l :u it y t }, and ( 4Φ G (u ) β u b Z = 4k In partiular, if b = 1, = 0, k = 0 and M u = 0 then )( R G b ). M A (4Φ G (u) β u )(R G 1). (16)
7 Proof. The proof follows by Theorem 2.1 with M = G b, then bounding u 2 G b and v t 2 G b via Lemma 4.1, and then using max t MA v it 2 G R G by equation (9). The upper bound of the theorem is more resilient to label imbalane, onept noise, and label noise than the bound in [8, Theorems 3.2, 4.1, and 4.2] (see equation (1)). For example, given the noisy barbell graph in Figure 3 but with k n noisy verties the bound (1) is O(kn) while the bound (15) with b = 1, = 1, and M u = 0 is O(k). A similar argument may be given for label imbalane. In the bound above, for easy interpretability, one may upper bound the resistane diameter R G by the geodesi diameter D G. However, the resistane diameter makes for a sharper bound in a number of natural situations. For example now onsider (a thik barbell) two mliques (one labeled 1, one 1 ) with l edges (l < m) between the liques. We observe between any two verties there are at least l edgedisjoint paths of length no more than five, therefore the resistane diameter is at most 5/l by the resistorsinparallel rule while the geodesi diameter is 3. Thus, for thik barbells if we use the geodesi diameter we have a mistake bound of 16l (substituting β u = 0, and R G 3 into (16)) while surprisingly with the resistane diameter the bound (substituting b = 1 4n, = 0, M u = 0, β u = 0, and R G 5/l into (15)) is independent of l and is Disussion In this paper, we have provided a bound on the performane of the pereptron on the graph in terms of strutural properties of the graph and its labeling whih are only indiretly dependent on the number of verties in the graph, in partiular, they depend on the ut size and the diameter. In the following, we ompare the pereptron with two other approahes. First, we ompare the pereptron with the graph kernel K 1 0 to the oneptually simpler knearest neighbors algorithm with either the graph geodesi distane or the resistane distane. In partiular, we prove the impossibility of bounding performane of knearest neighbors only in terms of the diameter and the ut size. Speifially, we give a parameterized family of graphs for whih the number of mistakes of the pereptron is upper bounded by a fixed onstant independent of the graph size while knearest neighbors provably inurs mistakes linearly in the graph size. Seond, we ompare the pereptron with the graph kernel K 1 0 with a simple appliation of the lassial halving algorithm [11]. Here, we onlude that the upper bound for the pereptron is better for graphs with a small diameter while the halving algorithm s upper bound is better for graphs with a large diameter. In the following, for simpliity we limit our disussion to binaryweighted graphs, noisefree data (see equation (16)) and upper bound the resistane diameter R G with the geodesi diameter D G (see equation (9)). 5.1 Knearest neighbors on the graph We onsider the knearest neighbors algorithms on the graph with both the resistane distane (see equation (7)) and the graph geodesi distane. The geodesi distane between two verties is the length of the shortest path between the two verties (reall the disussion in setion 3). In the following, we use the emphasis distane to refer simultaneously to both distanes. Now, onsider the family of O l,m,p of otopus graphs. An otopus graph (see Figure 5) onsists of a head whih is an llique (C (l) ) with verties denoted by 1,..., l, and a set of m tentales ({T i } m i=1 ), where eah tentale is a line graph of length p. The verties of tentale i are denoted by {t i,0, t i,1,..., t i,p }; the t i,0 are all identified as one vertex r whih ats as the root of the m tentales. There is an edge (the body) onneting root r to the vertex 1 on the head. Thus, this graph has diameter D = max(p 2, 2p) and there are l mp 1 verties in total; an otopus O m,p is balaned if l = mp 1. Note that the distane of every vertex in the head to every other vertex in the graph is no more than p 2, and every tentale tip t i,p is distane 2p to other tips t j,p : j i. We now argue that knearest neighbors may inur mistakes linear in the number of tentales. To this end, hoose p 3 and suppose we have the following online data sequene {( 1, 1), (t 1,p, 1), ( 2, 1), (t 2,p, 1),..., ( m, 1), (t m,p, 1)}. Note that knearest neighbors will make a mistake on every instane (t i,p, 1) and so, even assuming that it predits orretly on ( 1, 1) it will always make m mistakes. We now ontrast this result with the performane of the pereptron with the graph kernel K 1 0 (see equation (10)). By equation (16), the number of mistakes will be upper bounded by 10p 5 beause there is a ut of size 1 and the
8 diameter is 2p. Thus, for balaned otopi O m,p with p 3, as m grows the number of mistakes of the kernel pereptron will be bounded by a fixed onstant. Whereas distane knearest neighbors will inur mistakes linearly in m. 5.2 Halving algorithm We now ompare the performane of our algorithm to the lassial halving algorithm [11]. The halving algorithm operates by prediting on eah trial as the majority of the lassifiers in the onept lass whih have been onsistent over the trial sequene. Hene, the number of mistakes of the halving algorithm is upper bounded by the logarithm of the ardinality of the onept lass. Let KG k = {u { 1, 1}n : Φ G (u) = k} be the set all of all lassifiers with a ut size equal to k on a fixed graph G. The ardinality of KG k is upper bounded by ( ) n(n 1) k sine any lassifier (ut) in K k G an be uniquely identified by a hoie of k edges and 1 bit whih determines the sign of the verties in the same of partition (however we overount as not every set of edges determines a lassifier). The number of mistakes of the halving algorithm is upper bounded by O(k log n k ). For example, on a line graph with a ut size of 1 the halving algorithm has an upper bound of log n while the upper bound for the number of mistakes of the pereptron as given in equation (16) is 5n 5. Although the halving algorithm has a sharper bound on suh large diameter graphs as the line graph, it unfortunately has a logarithmi dependene on n. This ontrasts to the bound of the pereptron whih is essentially independent of n. Thus, the bound for the halving algorithm is roughly sharper on graphs with a diameter ω(log n k ), while the pereptron bound is roughly sharper on graphs with a diameter o(log n k ). We emphasize that this analysis of upper bounds is quite rough and sharper bounds for both algorithms ould be obtained for example, by inluding a term representing the minimal possible ut, that is, the minimum number of edges neessary to disonnet a graph. For the halving algorithm this would enable a better bound on the ardinality of KG k (see [13]). While, for the pereptron the larger the onnetivity of the graph, the weaker the diameter upper bound in Theorem 3.2 (see for example the disussion of thik barbells at the end of setion 4). Aknowledgments We wish to thank the anonymous reviewers for their useful omments. This work was supported by EPSRC Grant GR/T18707/01 and by the IST Programme of the European Community, under the PASCAL Network of Exellene IST Referenes [1] C. Gentile. The robustness of the pnorm algorithms. Mahine Learning, 53(3): , [2] A. Blum and S. Chawla. Learning from labeled and unlabeled data using graph minuts. In ICML 2002, pages Morgan Kaufmann, San Franiso, CA, [3] R. I. Kondor and J. Lafferty. Diffusion kernels on graphs and other disrete input spaes. In ICML 2002, pages Morgan Kaufmann, San Franiso, CA, [4] X. Zhu, Z. Ghahramani, and J. Lafferty. Semisupervised learning using gaussian fields and harmoni funtions. In ICML 2003, pages , [5] A. Smola and R.I. Kondor. Kernels and regularization on graphs. In COLT 2003, pages , [6] M. Belkin, I. Matveeva, and P. Niyogi. Regularization and semisupervised learning on large graphs. In COLT 2004, pages , Banff, Alberta, Springer. [7] T. Zhang and R. Ando. Analysis of spetral kernel design based semisupervised learning. In Y. Weiss, B. Shölkopf, and J. Platt, editors, NIPS 18, pages MIT Press, Cambridge, MA, [8] M. Herbster, M. Pontil, and L. Wainer. Online learning over graphs. In ICML 2005, pages , New York, NY, USA, ACM Press. [9] Y. Freund and R. E. Shapire. Large margin lassifiation using the pereptron algorithm. Mahine Learning, 37(3): , [10] D. Klein and M. Randić. Resistane distane. Journal of Mathematial Chemistry, 12(1):81 95, [11] J. M. Barzdin and R. V. Frievald. On the predition of general reursive funtions. Soviet Math. Doklady, 13: , [12] N. Aronszajn. Theory of reproduing kernels. Trans. Amer. Math. So., 68: , [13] D. Karger and C. Stein. A new approah to the minimum ut problem. JACM, 43(4): , 1996.
Complexity of Regularization RBF Networks
Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw
More informationMaximum Entropy and Exponential Families
Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It
More informationSensitivity Analysis in Markov Networks
Sensitivity Analysis in Markov Networks Hei Chan and Adnan Darwihe Computer Siene Department University of California, Los Angeles Los Angeles, CA 90095 {hei,darwihe}@s.ula.edu Abstrat This paper explores
More informationmax min z i i=1 x j k s.t. j=1 x j j:i T j
AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be
More informationPacking Plane Spanning Trees into a Point Set
Paking Plane Spanning Trees into a Point Set Ahmad Biniaz Alfredo Garía Abstrat Let P be a set of n points in the plane in general position. We show that at least n/3 plane spanning trees an be paked into
More informationOn Component Order Edge Reliability and the Existence of Uniformly Most Reliable Unicycles
Daniel Gross, Lakshmi Iswara, L. William Kazmierzak, Kristi Luttrell, John T. Saoman, Charles Suffel On Component Order Edge Reliability and the Existene of Uniformly Most Reliable Uniyles DANIEL GROSS
More informationA NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM
NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum
More informationarxiv:gr-qc/ v2 6 Feb 2004
Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this
More informationHankel Optimal Model Order Reduction 1
Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both
More informationLightpath routing for maximum reliability in optical mesh networks
Vol. 7, No. 5 / May 2008 / JOURNAL OF OPTICAL NETWORKING 449 Lightpath routing for maximum reliability in optial mesh networks Shengli Yuan, 1, * Saket Varma, 2 and Jason P. Jue 2 1 Department of Computer
More informationNonreversibility of Multiple Unicast Networks
Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast
More informationCMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017
CMSC 451: Leture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 Reading: Chapt 11 of KT and Set 54 of DPV Set Cover: An important lass of optimization problems involves overing a ertain domain,
More informationEffective Resistances for Ladder Like Chains
Effetive Resistanes for Ladder Like Chains Carmona, A., Eninas, A.M., Mitjana, M. May 9, 04 Abstrat Here we onsider a lass of generalized linear hains; that is, the ladder like hains as a perturbation
More informationChapter 8 Hypothesis Testing
Leture 5 for BST 63: Statistial Theory II Kui Zhang, Spring Chapter 8 Hypothesis Testing Setion 8 Introdution Definition 8 A hypothesis is a statement about a population parameter Definition 8 The two
More informationThe Effectiveness of the Linear Hull Effect
The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports
More information7 Max-Flow Problems. Business Computing and Operations Research 608
7 Max-Flow Problems Business Computing and Operations Researh 68 7. Max-Flow Problems In what follows, we onsider a somewhat modified problem onstellation Instead of osts of transmission, vetor now indiates
More informationSufficient Conditions for a Flexible Manufacturing System to be Deadlocked
Paper 0, INT 0 Suffiient Conditions for a Flexile Manufaturing System to e Deadloked Paul E Deering, PhD Department of Engineering Tehnology and Management Ohio University deering@ohioedu Astrat In reent
More informationModeling of Threading Dislocation Density Reduction in Heteroepitaxial Layers
A. E. Romanov et al.: Threading Disloation Density Redution in Layers (II) 33 phys. stat. sol. (b) 99, 33 (997) Subjet lassifiation: 6.72.C; 68.55.Ln; S5.; S5.2; S7.; S7.2 Modeling of Threading Disloation
More informationProbabilistic Graphical Models
Probabilisti Graphial Models David Sontag New York University Leture 12, April 19, 2012 Aknowledgement: Partially based on slides by Eri Xing at CMU and Andrew MCallum at UMass Amherst David Sontag (NYU)
More informationMillennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion
Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six
More informationRobust Recovery of Signals From a Structured Union of Subspaces
Robust Reovery of Signals From a Strutured Union of Subspaes 1 Yonina C. Eldar, Senior Member, IEEE and Moshe Mishali, Student Member, IEEE arxiv:87.4581v2 [nlin.cg] 3 Mar 29 Abstrat Traditional sampling
More informationV. Interacting Particles
V. Interating Partiles V.A The Cumulant Expansion The examples studied in the previous setion involve non-interating partiles. It is preisely the lak of interations that renders these problems exatly solvable.
More informationMethods of evaluating tests
Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed
More informationAdvanced Computational Fluid Dynamics AA215A Lecture 4
Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas
More informationDanielle Maddix AA238 Final Project December 9, 2016
Struture and Parameter Learning in Bayesian Networks with Appliations to Prediting Breast Caner Tumor Malignany in a Lower Dimension Feature Spae Danielle Maddix AA238 Final Projet Deember 9, 2016 Abstrat
More informationPredicting Graph Labels using Perceptron. Shuang Song
Predicting Graph Labels using Perceptron Shuang Song shs037@eng.ucsd.edu Online learning over graphs M. Herbster, M. Pontil, and L. Wainer, Proc. 22nd Int. Conf. Machine Learning (ICML'05), 2005 Prediction
More informationSensitivity analysis for linear optimization problem with fuzzy data in the objective function
Sensitivity analysis for linear optimization problem with fuzzy data in the objetive funtion Stephan Dempe, Tatiana Starostina May 5, 2004 Abstrat Linear programming problems with fuzzy oeffiients in the
More informationarxiv:math/ v4 [math.ca] 29 Jul 2006
arxiv:math/0109v4 [math.ca] 9 Jul 006 Contiguous relations of hypergeometri series Raimundas Vidūnas University of Amsterdam Abstrat The 15 Gauss ontiguous relations for F 1 hypergeometri series imply
More informationA Functional Representation of Fuzzy Preferences
Theoretial Eonomis Letters, 017, 7, 13- http://wwwsirporg/journal/tel ISSN Online: 16-086 ISSN Print: 16-078 A Funtional Representation of Fuzzy Preferenes Susheng Wang Department of Eonomis, Hong Kong
More informationA Characterization of Wavelet Convergence in Sobolev Spaces
A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat
More informationThe Unified Geometrical Theory of Fields and Particles
Applied Mathematis, 014, 5, 347-351 Published Online February 014 (http://www.sirp.org/journal/am) http://dx.doi.org/10.436/am.014.53036 The Unified Geometrial Theory of Fields and Partiles Amagh Nduka
More informationThe Laws of Acceleration
The Laws of Aeleration The Relationships between Time, Veloity, and Rate of Aeleration Copyright 2001 Joseph A. Rybzyk Abstrat Presented is a theory in fundamental theoretial physis that establishes the
More informationFlexible Word Design and Graph Labeling
Flexible Word Design and Graph Labeling Ming-Yang Kao Manan Sanghi Robert Shweller Abstrat Motivated by emerging appliations for DNA ode word design, we onsider a generalization of the ode word design
More informationSome Properties on Nano Topology Induced by Graphs
AASCIT Journal of anosiene 2017; 3(4): 19-23 http://wwwaasitorg/journal/nanosiene ISS: 2381-1234 (Print); ISS: 2381-1242 (Online) Some Properties on ano Topology Indued by Graphs Arafa asef 1 Abd El Fattah
More informationLecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont.
Stat60/CS94: Randomized Algorithms for Matries and Data Leture 7-09/5/013 Leture 7: Sampling/Projetions for Least-squares Approximation, Cont. Leturer: Mihael Mahoney Sribe: Mihael Mahoney Warning: these
More informationSINCE Zadeh s compositional rule of fuzzy inference
IEEE TRANSACTIONS ON FUZZY SYSTEMS, VOL. 14, NO. 6, DECEMBER 2006 709 Error Estimation of Perturbations Under CRI Guosheng Cheng Yuxi Fu Abstrat The analysis of stability robustness of fuzzy reasoning
More informationA Unified View on Multi-class Support Vector Classification Supplement
Journal of Mahine Learning Researh??) Submitted 7/15; Published?/?? A Unified View on Multi-lass Support Vetor Classifiation Supplement Ürün Doğan Mirosoft Researh Tobias Glasmahers Institut für Neuroinformatik
More informationEstimating the probability law of the codelength as a function of the approximation error in image compression
Estimating the probability law of the odelength as a funtion of the approximation error in image ompression François Malgouyres Marh 7, 2007 Abstrat After some reolletions on ompression of images using
More informationA Queueing Model for Call Blending in Call Centers
A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl
More informationWeighted K-Nearest Neighbor Revisited
Weighted -Nearest Neighbor Revisited M. Biego University of Verona Verona, Italy Email: manuele.biego@univr.it M. Loog Delft University of Tehnology Delft, The Netherlands Email: m.loog@tudelft.nl Abstrat
More informationAfter the completion of this section the student should recall
Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition
More informationAharonov-Bohm effect. Dan Solomon.
Aharonov-Bohm effet. Dan Solomon. In the figure the magneti field is onfined to a solenoid of radius r 0 and is direted in the z- diretion, out of the paper. The solenoid is surrounded by a barrier that
More informationDirectional Coupler. 4-port Network
Diretional Coupler 4-port Network 3 4 A diretional oupler is a 4-port network exhibiting: All ports mathed on the referene load (i.e. S =S =S 33 =S 44 =0) Two pair of ports unoupled (i.e. the orresponding
More informationAssessing the Performance of a BCI: A Task-Oriented Approach
Assessing the Performane of a BCI: A Task-Oriented Approah B. Dal Seno, L. Mainardi 2, M. Matteui Department of Eletronis and Information, IIT-Unit, Politenio di Milano, Italy 2 Department of Bioengineering,
More informationDiscrete Bessel functions and partial difference equations
Disrete Bessel funtions and partial differene equations Antonín Slavík Charles University, Faulty of Mathematis and Physis, Sokolovská 83, 186 75 Praha 8, Czeh Republi E-mail: slavik@karlin.mff.uni.z Abstrat
More informationarxiv:cond-mat/ v1 [cond-mat.str-el] 3 Aug 2006
arxiv:ond-mat/0608083v1 [ond-mat.str-el] 3 Aug 006 Raman sattering for triangular latties spin- 1 Heisenberg antiferromagnets 1. Introdution F. Vernay 1,, T. P. Devereaux 1, and M. J. P. Gingras 1,3 1
More informationLOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION
LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used
More informationConformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices
AAS 03-190 Conformal Mapping among Orthogonal, Symmetri, and Skew-Symmetri Matries Daniele Mortari Department of Aerospae Engineering, Texas A&M University, College Station, TX 77843-3141 Abstrat This
More informationTaste for variety and optimum product diversity in an open economy
Taste for variety and optimum produt diversity in an open eonomy Javier Coto-Martínez City University Paul Levine University of Surrey Otober 0, 005 María D.C. Garía-Alonso University of Kent Abstrat We
More informationLECTURE NOTES FOR , FALL 2004
LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as
More informationStability of alternate dual frames
Stability of alternate dual frames Ali Akbar Arefijamaal Abstrat. The stability of frames under perturbations, whih is important in appliations, is studied by many authors. It is worthwhile to onsider
More informationON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES
#A55 INTEGERS 3 (203) ON THE LEAST PRIMITIVE ROOT EPRESSIBLE AS A SUM OF TWO SQUARES Christopher Ambrose Mathematishes Institut, Georg-August Universität Göttingen, Göttingen, Deutshland ambrose@uni-math.gwdg.de
More informationControl Theory association of mathematics and engineering
Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology
More informationComputer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1
Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random
More informationthe following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined
How should a snake turn on ie: A ase study of the asymptoti isoholonomi problem Jianghai Hu, Slobodan N. Simić, and Shankar Sastry Department of Eletrial Engineering and Computer Sienes University of California
More informationOrdered fields and the ultrafilter theorem
F U N D A M E N T A MATHEMATICAE 59 (999) Ordered fields and the ultrafilter theorem by R. B e r r (Dortmund), F. D e l o n (Paris) and J. S h m i d (Dortmund) Abstrat. We prove that on the basis of ZF
More informationFrequency hopping does not increase anti-jamming resilience of wireless channels
Frequeny hopping does not inrease anti-jamming resiliene of wireless hannels Moritz Wiese and Panos Papadimitratos Networed Systems Seurity Group KTH Royal Institute of Tehnology, Stoholm, Sweden {moritzw,
More informationMulti-version Coding for Consistent Distributed Storage of Correlated Data Updates
Multi-version Coding for Consistent Distributed Storage of Correlated Data Updates Ramy E. Ali and Vivek R. Cadambe 1 arxiv:1708.06042v1 [s.it] 21 Aug 2017 Abstrat Motivated by appliations of distributed
More informationModel-based mixture discriminant analysis an experimental study
Model-based mixture disriminant analysis an experimental study Zohar Halbe and Mayer Aladjem Department of Eletrial and Computer Engineering, Ben-Gurion University of the Negev P.O.Box 653, Beer-Sheva,
More informationLecture Notes 4 MORE DYNAMICS OF NEWTONIAN COSMOLOGY
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physis Department Physis 8.286: The Early Universe Otober 1, 218 Prof. Alan Guth Leture Notes 4 MORE DYNAMICS OF NEWTONIAN COSMOLOGY THE AGE OF A FLAT UNIVERSE: We
More informationarxiv: v1 [physics.gen-ph] 5 Jan 2018
The Real Quaternion Relativity Viktor Ariel arxiv:1801.03393v1 [physis.gen-ph] 5 Jan 2018 In this work, we use real quaternions and the basi onept of the final speed of light in an attempt to enhane the
More informationJournal of Inequalities in Pure and Applied Mathematics
Journal of Inequalities in Pure and Applied Mathematis A NEW ARRANGEMENT INEQUALITY MOHAMMAD JAVAHERI University of Oregon Department of Mathematis Fenton Hall, Eugene, OR 97403. EMail: javaheri@uoregon.edu
More informationCounting Idempotent Relations
Counting Idempotent Relations Beriht-Nr. 2008-15 Florian Kammüller ISSN 1436-9915 2 Abstrat This artile introdues and motivates idempotent relations. It summarizes haraterizations of idempotents and their
More informationWavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013
Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it
More informationThe Second Postulate of Euclid and the Hyperbolic Geometry
1 The Seond Postulate of Eulid and the Hyperboli Geometry Yuriy N. Zayko Department of Applied Informatis, Faulty of Publi Administration, Russian Presidential Aademy of National Eonomy and Publi Administration,
More informationarxiv:cond-mat/ v1 [cond-mat.stat-mech] 16 Aug 2004
Computational omplexity and fundamental limitations to fermioni quantum Monte Carlo simulations arxiv:ond-mat/0408370v1 [ond-mat.stat-meh] 16 Aug 2004 Matthias Troyer, 1 Uwe-Jens Wiese 2 1 Theoretishe
More information1 sin 2 r = 1 n 2 sin 2 i
Physis 505 Fall 005 Homework Assignment #11 Solutions Textbook problems: Ch. 7: 7.3, 7.5, 7.8, 7.16 7.3 Two plane semi-infinite slabs of the same uniform, isotropi, nonpermeable, lossless dieletri with
More informationTHE classical noiseless index coding problem consists of. Lattice Index Coding. arxiv: v3 [cs.it] 7 Oct 2015
Lattie Index Coding Lakshmi Natarajan, Yi Hong, Senior Member, IEEE, and Emanuele Viterbo, Fellow, IEEE arxiv:40.6569v3 [s.it] 7 Ot 05 Abstrat The index oding problem involves a sender with K messages
More information). In accordance with the Lorentz transformations for the space-time coordinates of the same event, the space coordinates become
Relativity and quantum mehanis: Jorgensen 1 revisited 1. Introdution Bernhard Rothenstein, Politehnia University of Timisoara, Physis Department, Timisoara, Romania. brothenstein@gmail.om Abstrat. We first
More informationThe Hanging Chain. John McCuan. January 19, 2006
The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a
More informationUnderstanding Elementary Landscapes
Understanding Elementary Landsapes L. Darrell Whitley Andrew M. Sutton Adele E. Howe Department of Computer Siene Colorado State University Fort Collins, CO 853 {whitley,sutton,howe}@s.olostate.edu ABSTRACT
More informationWe will show that: that sends the element in π 1 (P {z 1, z 2, z 3, z 4 }) represented by l j to g j G.
1. Introdution Square-tiled translation surfaes are lattie surfaes beause they are branhed overs of the flat torus with a single branhed point. Many non-square-tiled examples of lattie surfaes arise from
More informationSoft BCL-Algebras of the Power Sets
International Journal of lgebra, Vol. 11, 017, no. 7, 39-341 HIKRI Ltd, www.m-hikari.om https://doi.org/10.1988/ija.017.7735 Soft BCL-lgebras of the Power Sets Shuker Mahmood Khalil 1 and bu Firas Muhamad
More informationHILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES
HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES L ERBE, A PETERSON AND S H SAKER Abstrat In this paper, we onsider the pair of seond-order dynami equations rt)x ) ) + pt)x
More informationEvaluation of effect of blade internal modes on sensitivity of Advanced LIGO
Evaluation of effet of blade internal modes on sensitivity of Advaned LIGO T0074-00-R Norna A Robertson 5 th Otober 00. Introdution The urrent model used to estimate the isolation ahieved by the quadruple
More informationThe shape of a hanging chain. a project in the calculus of variations
The shape of a hanging hain a projet in the alulus of variations April 15, 218 2 Contents 1 Introdution 5 2 Analysis 7 2.1 Model............................... 7 2.2 Extremal graphs.........................
More informationSURFACE WAVES OF NON-RAYLEIGH TYPE
SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh
More informationI F I G R e s e a r c h R e p o r t. Minimal and Hyper-Minimal Biautomata. IFIG Research Report 1401 March Institut für Informatik
I F I G R e s e a r h R e p o r t Institut für Informatik Minimal and Hyper-Minimal Biautomata Markus Holzer Seastian Jakoi IFIG Researh Report 1401 Marh 2014 Institut für Informatik JLU Gießen Arndtstraße
More informationConvergence of reinforcement learning with general function approximators
Convergene of reinforement learning with general funtion approximators assilis A. Papavassiliou and Stuart Russell Computer Siene Division, U. of California, Berkeley, CA 94720-1776 fvassilis,russellg@s.berkeley.edu
More informationFinal Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light
Final Review A Puzzle... Diretion of the Fore A point harge q is loated a fixed height h above an infinite horizontal onduting plane. Another point harge q is loated a height z (with z > h) above the plane.
More informationAverage Rate Speed Scaling
Average Rate Speed Saling Nikhil Bansal David P. Bunde Ho-Leung Chan Kirk Pruhs May 2, 2008 Abstrat Speed saling is a power management tehnique that involves dynamially hanging the speed of a proessor.
More informationError Bounds for Context Reduction and Feature Omission
Error Bounds for Context Redution and Feature Omission Eugen Bek, Ralf Shlüter, Hermann Ney,2 Human Language Tehnology and Pattern Reognition, Computer Siene Department RWTH Aahen University, Ahornstr.
More informationBilinear Formulated Multiple Kernel Learning for Multi-class Classification Problem
Bilinear Formulated Multiple Kernel Learning for Multi-lass Classifiation Problem Takumi Kobayashi and Nobuyuki Otsu National Institute of Advaned Industrial Siene and Tehnology, -- Umezono, Tsukuba, Japan
More informationCounting Arbitrary Subgraphs in Data Streams
Counting Arbitrary Subgraphs in Data Streams Daniel M. Kane 1, Kurt Mehlhorn, Thomas Sauerwald, and He Sun 1 Department of Mathematis, Stanford University, USA Max Plank Institute for Informatis, Germany
More informationarxiv:math.co/ v1 2 Aug 2006
A CHARACTERIZATION OF THE TUTTE POLYNOMIAL VIA COMBINATORIAL EMBEDDINGS OLIVIER BERNARDI arxiv:math.co/0608057 v1 2 Aug 2006 Abstrat. We give a new haraterization of the Tutte polynomial of graphs. Our
More information10.5 Unsupervised Bayesian Learning
The Bayes Classifier Maximum-likelihood methods: Li Yu Hongda Mao Joan Wang parameter vetor is a fixed but unknown value Bayes methods: parameter vetor is a random variable with known prior distribution
More informationc-perfect Hashing Schemes for Binary Trees, with Applications to Parallel Memories
-Perfet Hashing Shemes for Binary Trees, with Appliations to Parallel Memories (Extended Abstrat Gennaro Cordaso 1, Alberto Negro 1, Vittorio Sarano 1, and Arnold L.Rosenberg 2 1 Dipartimento di Informatia
More informationCombined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2
Sensor and Simulation Notes Note 53 3 May 8 Combined Eletri and Magneti Dipoles for Mesoband Radiation, Part Carl E. Baum University of New Mexio Department of Eletrial and Computer Engineering Albuquerque
More informationTight bounds for selfish and greedy load balancing
Tight bounds for selfish and greedy load balaning Ioannis Caragiannis Mihele Flammini Christos Kaklamanis Panagiotis Kanellopoulos Lua Mosardelli Deember, 009 Abstrat We study the load balaning problem
More informationELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW. P. М. Меdnis
ELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW P. М. Меdnis Novosibirs State Pedagogial University, Chair of the General and Theoretial Physis, Russia, 636, Novosibirs,Viljujsy, 8 e-mail: pmednis@inbox.ru
More informationThe Corpuscular Structure of Matter, the Interaction of Material Particles, and Quantum Phenomena as a Consequence of Selfvariations.
The Corpusular Struture of Matter, the Interation of Material Partiles, and Quantum Phenomena as a Consequene of Selfvariations. Emmanuil Manousos APM Institute for the Advanement of Physis and Mathematis,
More informationA NEW FLEXIBLE BODY DYNAMIC FORMULATION FOR BEAM STRUCTURES UNDERGOING LARGE OVERALL MOTION IIE THREE-DIMENSIONAL CASE. W. J.
A NEW FLEXIBLE BODY DYNAMIC FORMULATION FOR BEAM STRUCTURES UNDERGOING LARGE OVERALL MOTION IIE THREE-DIMENSIONAL CASE W. J. Haering* Senior Projet Engineer General Motors Corporation Warren, Mihigan R.
More informationLecture 3 - Lorentz Transformations
Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the
More informationLecture 15 (Nov. 1, 2017)
Leture 5 8.3 Quantum Theor I, Fall 07 74 Leture 5 (Nov., 07 5. Charged Partile in a Uniform Magneti Field Last time, we disussed the quantum mehanis of a harged partile moving in a uniform magneti field
More informationThe gravitational phenomena without the curved spacetime
The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,
More informationCoding for Random Projections and Approximate Near Neighbor Search
Coding for Random Projetions and Approximate Near Neighbor Searh Ping Li Department of Statistis & Biostatistis Department of Computer Siene Rutgers University Pisataay, NJ 8854, USA pingli@stat.rutgers.edu
More informationBäcklund Transformations: Some Old and New Perspectives
Bäklund Transformations: Some Old and New Perspetives C. J. Papahristou *, A. N. Magoulas ** * Department of Physial Sienes, Helleni Naval Aademy, Piraeus 18539, Greee E-mail: papahristou@snd.edu.gr **
More informationEinstein s Three Mistakes in Special Relativity Revealed. Copyright Joseph A. Rybczyk
Einstein s Three Mistakes in Speial Relativity Revealed Copyright Joseph A. Rybzyk Abstrat When the evidene supported priniples of eletromagneti propagation are properly applied, the derived theory is
More informationA Recursive Approach to the Kauffman Bracket
Applied Mathematis, 204, 5, 2746-2755 Published Online Otober 204 in SiRes http://wwwsirporg/journal/am http://ddoiorg/04236/am20457262 A Reursive Approah to the Kauffman Braet Abdul Rauf Nizami, Mobeen
More informationarxiv:gr-qc/ v7 14 Dec 2003
Propagation of light in non-inertial referene frames Vesselin Petkov Siene College, Conordia University 1455 De Maisonneuve Boulevard West Montreal, Quebe, Canada H3G 1M8 vpetkov@alor.onordia.a arxiv:gr-q/9909081v7
More information