527 research outputs found

    On a problem of Erd\H{o}s and Rothschild on edges in triangles

    Get PDF
    Erd\H{o}s and Rothschild asked to estimate the maximum number, denoted by H(N,C), such that every N-vertex graph with at least CN^2 edges, each of which is contained in at least one triangle, must contain an edge that is in at least H(N,C) triangles. In particular, Erd\H{o}s asked in 1987 to determine whether for every C>0 there is \epsilon >0 such that H(N,C) > N^\epsilon, for all sufficiently large N. We prove that H(N,C) = N^{O(1/log log N)} for every fixed C < 1/4. This gives a negative answer to the question of Erd\H{o}s, and is best possible in terms of the range for C, as it is known that every N-vertex graph with more than (N^2)/4 edges contains an edge that is in at least N/6 triangles.Comment: 8 page

    On two problems in graph Ramsey theory

    Get PDF
    We study two classical problems in graph Ramsey theory, that of determining the Ramsey number of bounded-degree graphs and that of estimating the induced Ramsey number for a graph with a given number of vertices. The Ramsey number r(H) of a graph H is the least positive integer N such that every two-coloring of the edges of the complete graph KNK_N contains a monochromatic copy of H. A famous result of Chv\'atal, R\"{o}dl, Szemer\'edi and Trotter states that there exists a constant c(\Delta) such that r(H) \leq c(\Delta) n for every graph H with n vertices and maximum degree \Delta. The important open question is to determine the constant c(\Delta). The best results, both due to Graham, R\"{o}dl and Ruci\'nski, state that there are constants c and c' such that 2^{c' \Delta} \leq c(\Delta) \leq 2^{c \Delta \log^2 \Delta}. We improve this upper bound, showing that there is a constant c for which c(\Delta) \leq 2^{c \Delta \log \Delta}. The induced Ramsey number r_{ind}(H) of a graph H is the least positive integer N for which there exists a graph G on N vertices such that every two-coloring of the edges of G contains an induced monochromatic copy of H. Erd\H{o}s conjectured the existence of a constant c such that, for any graph H on n vertices, r_{ind}(H) \leq 2^{c n}. We move a step closer to proving this conjecture, showing that r_{ind} (H) \leq 2^{c n \log n}. This improves upon an earlier result of Kohayakawa, Pr\"{o}mel and R\"{o}dl by a factor of \log n in the exponent.Comment: 18 page

    Inter-similarity between coupled networks

    Full text link
    Recent studies have shown that a system composed from several randomly interdependent networks is extremely vulnerable to random failure. However, real interdependent networks are usually not randomly interdependent, rather a pair of dependent nodes are coupled according to some regularity which we coin inter-similarity. For example, we study a system composed from an interdependent world wide port network and a world wide airport network and show that well connected ports tend to couple with well connected airports. We introduce two quantities for measuring the level of inter-similarity between networks (i) Inter degree-degree correlation (IDDC) (ii) Inter-clustering coefficient (ICC). We then show both by simulation models and by analyzing the port-airport system that as the networks become more inter-similar the system becomes significantly more robust to random failure.Comment: 4 pages, 3 figure

    Quantum Diffusion and Delocalization for Band Matrices with General Distribution

    Full text link
    We consider Hermitian and symmetric random band matrices HH in d1d \geq 1 dimensions. The matrix elements HxyH_{xy}, indexed by x,yΛZdx,y \in \Lambda \subset \Z^d, are independent and their variances satisfy \sigma_{xy}^2:=\E \abs{H_{xy}}^2 = W^{-d} f((x - y)/W) for some probability density ff. We assume that the law of each matrix element HxyH_{xy} is symmetric and exhibits subexponential decay. We prove that the time evolution of a quantum particle subject to the Hamiltonian HH is diffusive on time scales tWd/3t\ll W^{d/3}. We also show that the localization length of the eigenvectors of HH is larger than a factor Wd/6W^{d/6} times the band width WW. All results are uniform in the size \abs{\Lambda} of the matrix. This extends our recent result \cite{erdosknowles} to general band matrices. As another consequence of our proof we show that, for a larger class of random matrices satisfying xσxy2=1\sum_x\sigma_{xy}^2=1 for all yy, the largest eigenvalue of HH is bounded with high probability by 2+M2/3+ϵ2 + M^{-2/3 + \epsilon} for any ϵ>0\epsilon > 0, where M \deq 1 / (\max_{x,y} \sigma_{xy}^2).Comment: Corrected typos and some inaccuracies in appendix

    The critical window for the classical Ramsey-Tur\'an problem

    Get PDF
    The first application of Szemer\'edi's powerful regularity method was the following celebrated Ramsey-Tur\'an result proved by Szemer\'edi in 1972: any K_4-free graph on N vertices with independence number o(N) has at most (1/8 + o(1)) N^2 edges. Four years later, Bollob\'as and Erd\H{o}s gave a surprising geometric construction, utilizing the isoperimetric inequality for the high dimensional sphere, of a K_4-free graph on N vertices with independence number o(N) and (1/8 - o(1)) N^2 edges. Starting with Bollob\'as and Erd\H{o}s in 1976, several problems have been asked on estimating the minimum possible independence number in the critical window, when the number of edges is about N^2 / 8. These problems have received considerable attention and remained one of the main open problems in this area. In this paper, we give nearly best-possible bounds, solving the various open problems concerning this critical window.Comment: 34 page

    Problems and Results on Additive Properties of General Sequences IV

    Get PDF
    Let A={a1,a2,⋯}, a1<a2<⋯, be an infinite sequence of positive integers. One defines its counting function as A(n)=Card{a∈A;a≤n} (n=0,1,2,⋯), and the representation functions R1(n), R2(n), R3(n) (n=0,1,2,⋯), as being the number of representations of n in the form: (1) n=a+a′, a∈A, a′∈A, (2) n=a+a′, a<a′, a∈A, a′∈A, (3) n=a+a′, a≤a′, a∈A, a′∈A, respectively. Of course, for any n≥0, R1(n)=R2(n)+R3(n), and R3(n) is equal either to R2(n)+1, if n is even and n/2 belongs to A, or to R2(n), otherwise. In the first three parts of this series of papers [Erdős and Sárközy, Part I, Pacific J. Math. 118 (1985), no. 2, 347–357; MR0789175 (86j:11015); Part II, Acta Math. Hungar. 48 (1986), 201–211; MR0858398 (88c:11016); Part III, the authors, Studia Sci. Math. Hungar. 22 (1987), no. 1, 53–63], regularity properties of the asymptotic behavior of the function R1 were studied. In Parts IV and V the authors study monotonicity properties of the three functions R1,R2,R3. In Part IV, they prove first that the function R1 is monotone increasing from a certain point on (i.e., there exists an n0 withR1(n+1)≥R1(n) for n≥n0) if and only if the sequence A contains all the integers from a certain point on. The proof uses elementary but complex considerations on counting functions. Secondly, they show that R2 has a different behavior, by exhibiting a class of sequences A satisfying A(n <n−cn1/3 for all large n and such that R2 is monotone increasing from some point onwards. The third result proved in Part IV is that if A(n)=o(n/logn) then the functions R2 and R3 cannot be monotone increasing from a certain point on. Here, the proof is based on analytic properties of the generating function f(z)=∑a∈Aza (|z|<1), corresponding to the sequence A. Part V treats the monotonicity of R3. The main result is as follows: If (4) limn→+∞(n−A(n))/logn=+∞, then lim supN→+∞∑k=1N(R3(2k)−R3(2k+1))=+∞. (Thus, roughly speaking, ai+aj assumes more even values than odd ones.) This theorem implies, firstly, that under hypothesis (4), which is weaker than A(n)=o(n/logn), R3 cannot be monotone increasing from a certain point on, and, secondly, that if A is an infinite "Sidon sequence'' (also called a "B2-sequence'', i.e., a sequence such that R3(n)≤1 for all n), then there are infinitely many integers k such that 2k can be represented in the form 2k=a+a′, a∈A, a′∈A, but 2k+1=a+a′, a∈A, a′∈A, is impossible. Part V finishes with the construction of a sequence showing that the main result is almost best possible. The proofs in Part V are of the same nature as those in Part IV

    Robustness of a Network of Networks

    Full text link
    Almost all network research has been focused on the properties of a single network that does not interact and depends on other networks. In reality, many real-world networks interact with other networks. Here we develop an analytical framework for studying interacting networks and present an exact percolation law for a network of nn interdependent networks. In particular, we find that for nn Erd\H{o}s-R\'{e}nyi networks each of average degree kk, the giant component, PP_{\infty}, is given by P=p[1exp(kP)]nP_{\infty}=p[1-\exp(-kP_{\infty})]^n where 1p1-p is the initial fraction of removed nodes. Our general result coincides for n=1n=1 with the known Erd\H{o}s-R\'{e}nyi second-order phase transition for a single network. For any n2n \geq 2 cascading failures occur and the transition becomes a first-order percolation transition. The new law for PP_{\infty} shows that percolation theory that is extensively studied in physics and mathematics is a limiting case (n=1n=1) of a more general general and different percolation law for interdependent networks.Comment: 7 pages, 3 figure

    All scale-free networks are sparse

    Get PDF
    We study the realizability of scale free-networks with a given degree sequence, showing that the fraction of realizable sequences undergoes two first-order transitions at the values 0 and 2 of the power-law exponent. We substantiate this finding by analytical reasoning and by a numerical method, proposed here, based on extreme value arguments, which can be applied to any given degree distribution. Our results reveal a fundamental reason why large scale-free networks without constraints on minimum and maximum degree must be sparse.Comment: 4 pages, 2 figure

    Trapping in complex networks

    Full text link
    We investigate the trapping problem in Erdos-Renyi (ER) and Scale-Free (SF) networks. We calculate the evolution of the particle density ρ(t)\rho(t) of random walkers in the presence of one or multiple traps with concentration cc. We show using theory and simulations that in ER networks, while for short times ρ(t)exp(Act)\rho(t) \propto \exp(-Act), for longer times ρ(t)\rho(t) exhibits a more complex behavior, with explicit dependence on both the number of traps and the size of the network. In SF networks we reveal the significant impact of the trap's location: ρ(t)\rho(t) is drastically different when a trap is placed on a random node compared to the case of the trap being on the node with the maximum connectivity. For the latter case we find \rho(t)\propto\exp\left[-At/N^\frac{\gamma-2}{\gamma-1}\av{k}\right] for all γ>2\gamma>2, where γ\gamma is the exponent of the degree distribution P(k)kγP(k)\propto k^{-\gamma}.Comment: Appendix adde
    corecore