2013
DOI: 10.1016/j.geomphys.2013.02.004
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Noncommutative Riemannian geometry on graphs

Abstract: Abstract. We show that arising out of noncmmutatve geometry is a natural family of edge Laplacians on the edges of a graph. The family includes a canonical edge Laplacian associated to the graph, extending the usual graph Laplacian on vertices, and we find its spectrum. We show that for a connected graph its eigenvalues are strictly positive aside from one mandatory zero mode, and include all the vertex degrees. Our edge Laplacian is not the graph Laplacian on the line graph but rather it arises as the noncomm… Show more

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Cited by 48 publications
(88 citation statements)
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“…Here Ω 1 has basis {ω x→y } over C labelled by the arrows of the graph and differential df = ∑ x→y (f (y) − f (x))ω x→y . In this context a quantum metric [21] g = x→y g x→y ω x→y ⊗ ω y→x ∈ Ω 1 ⊗ C(X) Ω 1 requires weights g x→y ∈ R ∖ {0} for every edge and for every edge to be bi-directed (so there is an arrow in both directions). The calculus over C is compatible with complex conjugation on functions f * (x) = f (x) and ω * x→y = −ω y→x .…”
Section: 2mentioning
confidence: 99%
“…Here Ω 1 has basis {ω x→y } over C labelled by the arrows of the graph and differential df = ∑ x→y (f (y) − f (x))ω x→y . In this context a quantum metric [21] g = x→y g x→y ω x→y ⊗ ω y→x ∈ Ω 1 ⊗ C(X) Ω 1 requires weights g x→y ∈ R ∖ {0} for every edge and for every edge to be bi-directed (so there is an arrow in both directions). The calculus over C is compatible with complex conjugation on functions f * (x) = f (x) and ω * x→y = −ω y→x .…”
Section: 2mentioning
confidence: 99%
“…where in the graph case θ = ∑ x→y ω x→y and where α ∶ Ω 1 → Ω 1 ⊗ A Ω 1 and σ are bimodule maps (they commute with products by functions from either side). In this case, vanishing torsion and metric compatibility respectively become [22] (2.2) ∧ (id + σ) = 0, ∧α = 0…”
Section: Preliminaries: Quantum Geometric Formalismmentioning
confidence: 99%
“…The mathematics of quantum Riemannian geometry is simply more general than classical Riemannian geometry and includes discrete [27] as well as deformation examples. What is significant in this section is that whatever we find emerges from little else but the axioms applied to a square graph as 'manifold'.…”
Section: Quantum Gravity On a Square Graphmentioning
confidence: 99%