No Arabic abstract
A graph is a data structure composed of dots (i.e. vertices) and lines (i.e. edges). The dots and lines of a graph can be organized into intricate arrangements. The ability for a graph to denote objects and their relationships to one another allow for a surprisingly large number of things to be modeled as a graph. From the dependencies that link software packages to the wood beams that provide the framing to a house, most anything has a corresponding graph representation. However, just because it is possible to represent something as a graph does not necessarily mean that its graph representation will be useful. If a modeler can leverage the plethora of tools and algorithms that store and process graphs, then such a mapping is worthwhile. This article explores the world of graphs in computing and exposes situations in which graphical models are beneficial.
In this note we illustrate how common matrix approximation methods, such as random projection and random sampling, yield projection-cost-preserving sketches, as introduced in [FSS13, CEM+15]. A projection-cost-preserving sketch is a matrix approximation which, for a given parameter $k$, approximately preserves the distance of the target matrix to all $k$-dimensional subspaces. Such sketches have applications to scalable algorithms for linear algebra, data science, and machine learning. Our goal is to simplify the presentation of proof techniques introduced in [CEM+15] and [CMM17] so that they can serve as a guide for future work. We also refer the reader to [CYD19], which gives a similar simplified exposition of the proof covered in Section 2.
Let $P$ be a set (called points), $Q$ be a set (called queries) and a function $ f:Ptimes Qto [0,infty)$ (called cost). For an error parameter $epsilon>0$, a set $Ssubseteq P$ with a emph{weight function} $w:P rightarrow [0,infty)$ is an $epsilon$-coreset if $sum_{sin S}w(s) f(s,q)$ approximates $sum_{pin P} f(p,q)$ up to a multiplicative factor of $1pmepsilon$ for every given query $qin Q$. We construct coresets for the $k$-means clustering of $n$ input points, both in an arbitrary metric space and $d$-dimensional Euclidean space. For Euclidean space, we present the first coreset whose size is simultaneously independent of both $d$ and $n$. In particular, this is the first coreset of size $o(n)$ for a stream of $n$ sparse points in a $d ge n$ dimensional space (e.g. adjacency matrices of graphs). We also provide the first generalizations of such coresets for handling outliers. For arbitrary metric spaces, we improve the dependence on $k$ to $k log k$ and present a matching lower bound. For $M$-estimator clustering (special cases include the well-known $k$-median and $k$-means clustering), we introduce a new technique for converting an offline coreset construction to the streaming setting. Our method yields streaming coreset algorithms requiring the storage of $O(S + k log n)$ points, where $S$ is the size of the offline coreset. In comparison, the previous state-of-the-art was the merge-and-reduce technique that required $O(S log^{2a+1} n)$ points, where $a$ is the exponent in the offline constructions dependence on $epsilon^{-1}$. For example, combining our offline and streaming results, we produce a streaming metric $k$-means coreset algorithm using $O(epsilon^{-2} k log k log n)$ points of storage. The previous state-of-the-art required $O(epsilon^{-4} k log k log^{6} n)$ points.
We study the problem of finding a mapping $f$ from a set of points into the real line, under ordinal triple constraints. An ordinal constraint for a triple of points $(u,v,w)$ asserts that $|f(u)-f(v)|<|f(u)-f(w)|$. We present an approximation algorithm for the dense case of this problem. Given an instance that admits a solution that satisfies $(1-varepsilon)$-fraction of all constraints, our algorithm computes a solution that satisfies $(1-O(varepsilon^{1/8}))$-fraction of all constraints, in time $O(n^7) + (1/varepsilon)^{O(1/varepsilon^{1/8})} n$.
Cathodoluminescence measurements on single InGaN/GaN quantum dots (QDs) are reported. Complex spectra with up to five emission lines per QD are observed. The lines are polarized along the orthogonal crystal directions [1 1 -2 0] and [-1 1 0 0]. Realistic eight-band k.p electronic structure calculations show that the polarization of the lines can be explained by excitonic recombinations involving hole states which are either formed by the A or the B valence band.
Systematic constructions of MDS self-dual codes is widely concerned. In this paper, we consider the constructions of MDS Euclidean self-dual codes from short length. Indeed, the exact constructions of MDS Euclidean self-dual codes from short length ($n=3,4,5,6$) are given. In general, we construct more new of $q$-ary MDS Euclidean self-dual codes from MDS self-dual codes of known length via generalized Reed-Solomon (GRS for short) codes and extended GRS codes.