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Approaches to Quantum Gravity

Approaches to Quantum Gravity

Approaches to Quantum Gravity

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New directions in background independent <strong>Quantum</strong> <strong>Gravity</strong> 1319.2 <strong>Quantum</strong> Causal His<strong>to</strong>riesA <strong>Quantum</strong> Causal His<strong>to</strong>ry is a locally finite directed graph of finite-dimensionalquantum systems. We start by giving the properties of the directed graph and theassignment of quantum systems <strong>to</strong> its vertices and appropriate opera<strong>to</strong>rs <strong>to</strong> itsedges. The addition of three axioms ensures that the properties of a given graphare reflected in the flow of physical information in the corresponding quantumopera<strong>to</strong>rs and completes the definition of a <strong>Quantum</strong> Causal His<strong>to</strong>ry. 2Let Ɣ be a directed graph with vertices x ∈ V (Ɣ) and directed edges e ∈ E(Ɣ).The source s(e) and range r(e) of an edge e are, respectively, the initial and finalvertex of e. A (finite) path w = e k ···e 1 in Ɣ is a sequence of edges of Ɣ such thatr(e i ) = s(e i+1 ) for 1 ≤ i < k.Ifs(w) = r(w) then we say w is a cycle. We requirethat Ɣ has no cycles.If there exists a path w such that s(w) = x and r(w) = y let us write x ≤ y forthe associated partial ordering. We call such vertices related. Otherwise, they areunrelated. Weusex ∼ z <strong>to</strong> denote that x and z are unrelated. Given any x ≤ y,we require that there are finitely many z ∈ V (Ɣ) such that x ≤ z ≤ y. Thisisthecondition of local finiteness.Definition 1 Parallel set, complete source, complete range, complete pair.A parallel set ξ ⊆ E(Ɣ) is defined by the property that x ∼ y whenever x, y ∈ ξ.A parallel set ξ is a complete source of x if all paths w with r(w) ≡ x have s(w) ∈ξ. Conversely, a parallel set ζ is a complete range of x if all paths w with sources(w) ≡ x have range in ζ ,r(w) ∈ ζ . Two parallel sets ξ and ζ are a completepair if all paths w that start in ξ s(w) ∈ ξ end up in ζ ,r(w) ∈ ζ and the reverse.For example, in the directed graphξ 1 is a complete source for y while the parallel sets ξ 2 and η are not. The sets η andɛ are a complete pair.We now wish <strong>to</strong> associate quantum systems <strong>to</strong> the graph. The construction ofa <strong>Quantum</strong> Causal His<strong>to</strong>ry starts with a directed graph Ɣ and assigns <strong>to</strong> every2 The abstract form of a <strong>Quantum</strong> Causal His<strong>to</strong>ry based on a directed graph that we follow here was given byKribs [15], based on the original definition in [22] and[11].

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