2,290 research outputs found

    Inapproximability of the Standard Pebble Game and Hard to Pebble Graphs

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    Pebble games are single-player games on DAGs involving placing and moving pebbles on nodes of the graph according to a certain set of rules. The goal is to pebble a set of target nodes using a minimum number of pebbles. In this paper, we present a possibly simpler proof of the result in [CLNV15] and strengthen the result to show that it is PSPACE-hard to determine the minimum number of pebbles to an additive n1/3ϵn^{1/3-\epsilon} term for all ϵ>0\epsilon > 0, which improves upon the currently known additive constant hardness of approximation [CLNV15] in the standard pebble game. We also introduce a family of explicit, constant indegree graphs with nn nodes where there exists a graph in the family such that using constant kk pebbles requires Ω(nk)\Omega(n^k) moves to pebble in both the standard and black-white pebble games. This independently answers an open question summarized in [Nor15] of whether a family of DAGs exists that meets the upper bound of O(nk)O(n^k) moves using constant kk pebbles with a different construction than that presented in [AdRNV17].Comment: Preliminary version in WADS 201

    General Connectivity Distribution Functions for Growing Networks with Preferential Attachment of Fractional Power

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    We study the general connectivity distribution functions for growing networks with preferential attachment of fractional power, Πikα\Pi_{i} \propto k^{\alpha}, using the Simon's method. We first show that the heart of the previously known methods of the rate equations for the connectivity distribution functions is nothing but the Simon's method for word problem. Secondly, we show that the case of fractional α\alpha the ZZ-transformation of the rate equation provides a fractional differential equation of new type, which coincides with that for PA with linear power, when α=1\alpha = 1. We show that to solve such a fractional differential equation we need define a transidental function Υ(a,s,c;z)\Upsilon (a,s,c;z) that we call {\it upsilon function}. Most of all previously known results are obtained consistently in the frame work of a unified theory.Comment: 10 page

    The Definition and Measurement of the Topological Entropy per Unit Volume in Parabolic PDE's

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    We define the topological entropy per unit volume in parabolic PDE's such as the complex Ginzburg-Landau equation, and show that it exists, and is bounded by the upper Hausdorff dimension times the maximal expansion rate. We then give a constructive implementation of a bound on the inertial range of such equations. Using this bound, we are able to propose a finite sampling algorithm which allows (in principle) to measure this entropy from experimental data.Comment: 26 pages, 1 small figur

    Absence of reflection as a function of the coupling constant

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    We consider solutions of the one-dimensional equation u+(Q+λV)u=0-u'' +(Q+ \lambda V) u = 0 where Q:RRQ: \mathbb{R} \to \mathbb{R} is locally integrable, V:RRV : \mathbb{R} \to \mathbb{R} is integrable with supp(V)[0,1](V) \subset [0,1], and λR\lambda \in \mathbb{R} is a coupling constant. Given a family of solutions {uλ}λR\{u_{\lambda} \}_{\lambda \in \mathbb{R}} which satisfy uλ(x)=u0(x)u_{\lambda}(x) = u_0(x) for all x<0x<0, we prove that the zeros of b(λ):=W[u0,uλ]b(\lambda) := W[u_0, u_{\lambda}], the Wronskian of u0u_0 and uλu_{\lambda}, form a discrete set unless V0V \equiv 0. Setting Q(x):=EQ(x) := -E, one sees that a particular consequence of this result may be stated as: if the fixed energy scattering experiment u+λVu=Eu-u'' + \lambda V u = Eu gives rise to a reflection coefficient which vanishes on a set of couplings with an accumulation point, then V0V \equiv 0.Comment: To appear in Journal of Mathematical Physic
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