12,090 research outputs found

    Maximal antichains of minimum size

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    Let nβ©Ύ4n\geqslant 4 be a natural number, and let KK be a set KβŠ†[n]:=1,2,...,nK\subseteq [n]:={1,2,...,n}. We study the problem to find the smallest possible size of a maximal family A\mathcal{A} of subsets of [n][n] such that A\mathcal{A} contains only sets whose size is in KK, and AβŠ†ΜΈBA\not\subseteq B for all A,BβŠ†A{A,B}\subseteq\mathcal{A}, i.e. A\mathcal{A} is an antichain. We present a general construction of such antichains for sets KK containing 2, but not 1. If 3∈K3\in K our construction asymptotically yields the smallest possible size of such a family, up to an o(n2)o(n^2) error. We conjecture our construction to be asymptotically optimal also for 3∉K3\not\in K, and we prove a weaker bound for the case K=2,4K={2,4}. Our asymptotic results are straightforward applications of the graph removal lemma to an equivalent reformulation of the problem in extremal graph theory which is interesting in its own right.Comment: fixed faulty argument in Section 2, added reference

    Pointwise ergodic theorem for locally countable quasi-pmp graphs

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    We prove a pointwise ergodic theorem for quasi-probability-measure-preserving (quasi-pmp) locally countable measurable graphs, analogous to pointwise ergodic theorems for group actions, replacing the group with a Schreier graph of the action. For any quasi-pmp graph, the theorem gives an increasing sequence of Borel subgraphs with finite connected components along which the averages of L1L^1 functions converge to their expectations. Equivalently, it states that any (not necessarily pmp) locally countable Borel graph on a standard probability space contains an ergodic hyperfinite subgraph. The pmp version of this theorem was first proven by R. Tucker-Drob using probabilistic methods. Our proof is different: it is descriptive set theoretic and applies more generally to quasi-pmp graphs. Among other things, it involves introducing a graph invariant, a method of producing finite equivalence subrelations with large domain, and a simple method of exploiting nonamenability of a measured graph. The non-pmp setting additionally requires a new gadget for analyzing the interplay between the underlying cocycle and the graph.Comment: Added to the introduction a discussion of existing results about pointwise ergodic theorems for quasi-action

    Discrete chain graph models

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    The statistical literature discusses different types of Markov properties for chain graphs that lead to four possible classes of chain graph Markov models. The different models are rather well understood when the observations are continuous and multivariate normal, and it is also known that one model class, referred to as models of LWF (Lauritzen--Wermuth--Frydenberg) or block concentration type, yields discrete models for categorical data that are smooth. This paper considers the structural properties of the discrete models based on the three alternative Markov properties. It is shown by example that two of the alternative Markov properties can lead to non-smooth models. The remaining model class, which can be viewed as a discrete version of multivariate regressions, is proven to comprise only smooth models. The proof employs a simple change of coordinates that also reveals that the model's likelihood function is unimodal if the chain components of the graph are complete sets.Comment: Published in at http://dx.doi.org/10.3150/08-BEJ172 the Bernoulli (http://isi.cbs.nl/bernoulli/) by the International Statistical Institute/Bernoulli Society (http://isi.cbs.nl/BS/bshome.htm

    On Saturated kk-Sperner Systems

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    Given a set XX, a collection FβŠ†P(X)\mathcal{F}\subseteq\mathcal{P}(X) is said to be kk-Sperner if it does not contain a chain of length k+1k+1 under set inclusion and it is saturated if it is maximal with respect to this property. Gerbner et al. conjectured that, if ∣X∣|X| is sufficiently large with respect to kk, then the minimum size of a saturated kk-Sperner system FβŠ†P(X)\mathcal{F}\subseteq\mathcal{P}(X) is 2kβˆ’12^{k-1}. We disprove this conjecture by showing that there exists Ξ΅>0\varepsilon>0 such that for every kk and ∣X∣β‰₯n0(k)|X| \geq n_0(k) there exists a saturated kk-Sperner system FβŠ†P(X)\mathcal{F}\subseteq\mathcal{P}(X) with cardinality at most 2(1βˆ’Ξ΅)k2^{(1-\varepsilon)k}. A collection FβŠ†P(X)\mathcal{F}\subseteq \mathcal{P}(X) is said to be an oversaturated kk-Sperner system if, for every S∈P(X)βˆ–FS\in\mathcal{P}(X)\setminus\mathcal{F}, Fβˆͺ{S}\mathcal{F}\cup\{S\} contains more chains of length k+1k+1 than F\mathcal{F}. Gerbner et al. proved that, if ∣X∣β‰₯k|X|\geq k, then the smallest such collection contains between 2k/2βˆ’12^{k/2-1} and O(log⁑kk2k)O\left(\frac{\log{k}}{k}2^k\right) elements. We show that if ∣X∣β‰₯k2+k|X|\geq k^2+k, then the lower bound is best possible, up to a polynomial factor.Comment: 17 page

    Instanton--anti-instanton pair induced contributions to Re+eβˆ’β†’hadronsR_{e^+e^-\to hadrons} and RΟ„β†’hadronsR_{\tau \to hadrons}

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    The instanton--anti-instanton pair induced asymptotics of perturbation theory expansion for the cross section of electron--positron pair annihilation to hadrons and hadronic width of Ο„\tau-lepton was found. For Nf=NcN_f = N_c the nonperturbative instanton contribution is finite and may be calculated without phenomenological input. The instanton induced peturbative asymptotics was shown to be enhanced as (n+10)!(n+10)! and in the intermediate region n<15n<15 may exceed the renormalon contribution. Unfortunately, the analysis of ∼1/n\sim 1/n corrections shows that for n∼10n \sim 10 the obtained asymptotic expressions are at best only the order of magnitude estimate. The asymptotic series for Re+eβˆ’β†’hadronsR_{e^+ e^- \rightarrow hadrons} , though obtained formally for Nf=NcN_f =N_c, is valid up to energies ∼15\sim 15Gev. The instanton--anti-instanton pair nonperturbative contribution to RΟ„β†’hadronsR_{\tau \rightarrow hadrons} blows up. On the one hand, this means that instantons could not be considered {\it ab--initio} at such energies. On the other hand, this result casts a strong doubt upon the possibility to determine the Ξ±s\alpha_s from the Ο„\tau--lepton width.Comment: 22 pages, latex, no figure
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