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{{Short description|Graph where every edge is in one triangle}}
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In [[graph theory]], a '''locally linear graph''' is an [[undirected graph]] in which every edge belongs to exactly one triangle. Equivalently, for each vertex of the graph, its [[neighborhood (graph theory)|neighbors]] are each adjacent to exactly one other neighbor. That is, locally (from the point of view of any one vertex) the rest of the graph looks like a [[perfect matching]].{{r|f}} Locally linear graphs have also been called locally matched graphs.{{r|lpv}} More technically, the triangles of any locally linear graph form the [[hyperedge]]s of a triangle-free 3-uniform linear [[hypergraph]], and they form the blocks of certain [[Steiner system|partial Steiner triple systems]]; and the locally linear graphs are exactly the [[Gaifman graph]]s of these hypergraphs or partial Steiner systems.
Many constructions for locally linear graphs are known. Examples of locally linear graphs include the [[triangular cactus graph]]s, the [[line graph]]s of 3-regular [[triangle-free graph]]s, and the [[Cartesian product of graphs|Cartesian products]] of smaller locally linear graphs. Certain [[Kneser graph]]s, and certain [[strongly regular graph]]s, are also locally linear.
==Constructions and examples==▼
[[File:Cuboctahedron.jpg|thumb|The [[cuboctahedron]], a planar locally linear graph that can be formed as the line graph of a cube or by gluing antiprisms onto the inside and outside faces of a 4-cycle]]▼
===Gluing and products===
[[File:Friendship graphs.svg|thumb|[[Friendship graph]]s]]
The [[friendship graph]]s, graphs formed by gluing together a collection of triangles at a single shared vertex, are locally linear. They are the only finite graphs having the stronger property that every pair of vertices (adjacent or not) share exactly one common neighbor.{{r|ers}} More generally every [[Cactus graph#Triangular cactus|triangular cactus graph]], a graph
Let <math>G</math> and <math>H</math> be any two locally linear graphs, select a triangle from each of them, and glue the two graphs by merging together corresponding pairs of vertices in the two selected triangles. Then the resulting graph remains locally linear.{{r|z}}
The [[Cartesian product of graphs|Cartesian product]] of any two locally linear graphs remains locally linear, because any triangles in the product come from triangles in one or the other factors. For instance, the nine-vertex [[Paley graph]] (the graph of the [[3-3 duoprism]]) is the Cartesian product of two triangles.{{r|f}} The [[Hamming graph]] <math>H(d,3)</math> is a Cartesian product of <math>d</math> triangles, and again is locally linear.{{r|djlp}}
===
▲[[File:Cuboctahedron.
A more complicated expansion process applies to [[planar graph]]s. Let <math>G</math> be a planar graph embedded in the plane in such a way that every face is a quadrilateral, such as the graph of a cube
The removed 4-cycle of this construction can be seen on the cuboctahedron as a cycle of four diagonals of its square faces, bisecting the polyhedron.
===Algebraic constructions===
Locally linear graphs can also be constructed from progression-free sets of numbers.
Let <math>p</math> be a prime number, and let <math>A</math> be a subset of the numbers modulo <math>p</math> such that no three members of <math>A</math> form an [[arithmetic progression]] modulo <math>p</math>. (That is, <math>A</math> is a [[Salem–Spencer set]] modulo <math>p</math>.)
The triangles in a locally linear graph can be equivalently thought of as forming a 3-uniform [[hypergraph]]. Such a hypergraph must be linear, meaning that no two of its hyperedges (the triangles) can share more than one vertex. The locally linear graph itself is the [[Gaifman graph]] of the hypergraph, the graph of pairs of vertices that belong to a common hyperedge. In this view it makes sense to talk about the [[girth (graph theory)|girth]] of the hypergraph. In graph terms, this is the length of the shortest cycle that is not one of the triangles of the graph. An algebraic construction based on [[polarity graph]]s (also called Brown graphs) has been used, in this context, to find dense locally linear graphs that have no 4-cycles; their hypergraph girth is five. A polarity graph is defined from a [[finite projective plane]], and a [[Correlation (projective geometry)|polarity]], an incidence-preserving bijection between its points and its lines. The vertices of the polarity graph are points, and an edge connects two points whenever one is polar to a line containing the other. More algebraically, the vertices of the same graph can be represented by [[homogeneous coordinate]]s: these are triples of values <math>(x,y,z)</math> from a [[finite field]], not all zero, where two triples define the same point in the plane whenever they are scalar multiples of each other. Two points, represented by triples in this way, are adjacent when their [[inner product]] is zero. The polarity graph for a finite field of odd order <math>q</math> has <math>q^2+q+1</math> vertices, of which <math>q+1</math> are self-adjacent and do not belong to any triangles. When these are removed, the result is a locally linear graph with <math>q^2</math> vertices, <math>\bigl(\tfrac12+o(1)\bigr)q^3</math> edges, and hypergraph girth five, giving the maximum possible number of edges for a locally linear graph of this girth up to lower-order terms.{{r|lv}}
==Regularity==
===Regular graphs with few vertices===
===Regular and strongly regular graphs===▼
▲Every locally linear graph must have even [[degree (graph theory)|degree]] at each vertex, because the edges at each vertex can be paired up into triangles. The Cartesian product of two locally linear regular graphs is again locally linear and regular, with degree equal to the sum of the degrees of the factors. Therefore, there exist regular locally linear graphs of every even degree.{{r|f}}
The <math>2r</math>-regular locally linear graphs must have at least <math>6r-3</math> vertices, because there are this many vertices among any triangle and its neighbors alone. (No two vertices of the triangle can share a neighbor without violating local linearity.) Regular graphs with exactly this many vertices are possible only when <math>r</math> is 1, 2, 3, or 5, and are uniquely defined for each of these four cases. The four regular graphs meeting this bound on the number of vertices are the 3-vertex 2-regular triangle <math>K_3</math>, the 9-vertex 4-regular Paley graph, the 15-vertex 6-regular Kneser graph <math>KG_{6,2}</math>, and the 27-vertex 10-regular [[complement graph]] of the [[Schläfli graph]]. The final 27-vertex 10-regular graph also represents the [[intersection graph]] of the 27 lines on a [[cubic surface]].{{r|lpv}}
A [[strongly regular graph]] can be characterized by a quadruple of parameters <math>(n,k,\lambda,\mu)</math> where <math>n</math> is the number of vertices, <math>k</math> is the number of incident edges per vertex, <math>\lambda</math> is the number of shared neighbors for every adjacent pair of vertices, and <math>\mu</math> is the number of shared neighbors for every non-adjacent pair of vertices. When <math>\lambda=1</math> the graph is locally linear. The locally linear graphs already mentioned above that are strongly regular graphs and their parameters are{{r|mak}}
*the triangle (3,2,1,0),
*the nine-vertex Paley graph (9,4,1,2),
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Other potentially-valid combinations with <math>\lambda=1</math> include (99,14,1,2) and (115,18,1,3) but it is unknown whether strongly regular graphs with those parameters exist.{{r|mak}} The question of the existence of a strongly regular graph with parameters (99,14,1,2) is known as [[Conway's 99-graph problem]], and [[John Horton Conway]] has offered a $1000 prize for its solution.{{r|zd}}
===Distance-regular graphs===
There are finitely many [[distance-regular graph]]s of degree 4 or 6 that are locally linear. Beyond the strongly regular graphs of the same degrees, they also include the line graph of the Petersen graph, the Hamming graph <math>H(3,3)</math>, and the [[Bipartite half|halved]] [[Foster graph]].{{r|hns}}
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[[File:Dense planar locally linear.svg|thumb|The densest possible locally linear planar graphs are formed by gluing an antiprism (red vertices and black edges) into each quadrilateral face of a planar graph (blue vertices and dashed yellow edges)]]
{{main|Ruzsa–Szemerédi problem}}
One formulation of the [[Ruzsa–Szemerédi problem]] asks for the maximum number of edges in an <math>n</math>-vertex locally linear graph. As [[Imre Z. Ruzsa]] and [[Endre Szemerédi]] proved, this maximum number is <math>o(n^2)</math> but is <math>\Omega(n^{2-\varepsilon})</math> for every <math>\varepsilon>0</math>. The construction of locally linear graphs from progression-free sets leads to the densest known locally linear graphs, with <math>n^2/\exp O(\sqrt{\log n})</math> edges. (In these formulas, <math>o</math>, <math>\Omega</math>, and <math>O</math> are examples of [[little o notation]], [[big Omega notation]], and [[big O notation]], respectively.){{r|rs}}
Among [[planar graph]]s, the maximum number of edges in a locally linear graph with <math>n</math> vertices is <math>\tfrac{12}{5}(n-2)</math>. The graph of the [[cuboctahedron]] is the first in an infinite sequence of [[polyhedral graph]]s with <math>n=5k+2</math> vertices and <math>\tfrac{12}{5}(n-2)=12k</math> edges, for <math>k=2,3,\dots</math>, constructed by expanding the quadrilateral faces of <math>K_{2,k}</math> into antiprisms. These examples show that
Every locally linear graph has the property that it remains connected after any matching is removed from it, because in any path through the graph, each matched edge can be replaced by the other two edges of its triangle. Among the graphs with this property, the least dense are the triangular cactus graphs, which are also the least dense locally linear graphs.{{r|fp}}
==Applications==
One application of locally linear graphs occurs in the formulation of [[Greechie diagram]]s, which are used in [[quantum logic]] to help determine whether certain [[Hilbert space]] equations can be inferred from each other. In this application, the triangles of locally linear graphs form the blocks of Greechie diagrams with block size three. The Greechie diagrams corresponding to lattices come from the locally linear graphs of hypergraph girth five or more,{{r|mmp}} as constructed for instance from polarity graphs.{{r|lv}}
A combination of random sampling and a [[graph removal lemma]] can be used to find large high-girth 3-uniform hypergraphs within arbitrary 3-uniform linear hypergraphs or partial Steiner triple systems. This method can then be used to prove [[asymptotic analysis|asymptotically tight]] lower bounds on the [[independence number]] of 3-uniform linear hypergraphs and partial Steiner triple systems.{{r|hy}}
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