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・ Causal dynamical triangulation
・ Causal fermion system
・ Causal filter
・ Causal graph
・ Causal inference
・ Causal layered analysis
・ Causal loop
・ Causal loop diagram
・ Causal Markov condition
・ Causal model
・ Causal patch
・ Causal perturbation theory
・ Causal plane
・ Causal reasoning
・ Causal research
Causal sets
・ Causal structure
・ Causal system
・ Causal theory
・ Causal theory of knowledge
・ Causal theory of reference
・ Causal thinking
・ Causalism
・ Causality
・ Causality (disambiguation)
・ Causality (physics)
・ Causality conditions
・ Causanagh
・ Causantín mac Cináeda
・ Causantín mac Fergusa


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Causal sets : ウィキペディア英語版
Causal sets

The causal sets programme is an approach to quantum gravity. Its founding principles are that spacetime is fundamentally discrete and that spacetime events are related by a partial order. This partial order has the physical meaning of the causality relations between spacetime events.
The programme is based on a theorem〔D. Malament, ''(The class of continuous timelike curves determines the topology of spacetime )'', Journal of Mathematical Physics, July 1977, Volume 18, Issue 7, pp. 1399-1404〕 by David Malament that states that if there is a bijective map between two past and future distinguishing spacetimes that preserves their causal structure then the map is a conformal isomorphism. The conformal factor that is left undetermined is related to the volume of regions in the spacetime. This volume factor can be recovered by specifying a volume element for each spacetime point. The volume of a spacetime region could then be found by counting the number of points in that region.
Causal sets was initiated by Rafael Sorkin who continues to be the main proponent of the programme. He has coined the slogan "Order + Number = Geometry" to characterise the above argument. The programme provides a theory in which spacetime is fundamentally discrete while retaining local Lorentz invariance.
== Definition ==
A causal set (or causet) is a set C with a partial order relation \preceq that is
* Reflexive: For all x \in C, we have x \preceq x .
* Antisymmetric: For all x, y \in C, we have x \preceq y \preceq x \implies x = y.
* Transitive: For all x, y, z \in C, we have x \preceq y \preceq z implies x \preceq z .
* Locally finite: For all x, z \in C, we have card (\) < \infty .

Here card(A) denotes the cardinality of a set A. We'll write x \prec y if x \preceq y and x \neq y.
The set C represents the set of spacetime events and the order relation \preceq represents the causal relationship between events (see causal structure for the analogous idea in a Lorentzian manifold).
Although this definition uses the reflexive convention we could have chosen the irreflexive convention in which the order relation is irreflexive. The causal relation of a Lorentzian manifold (without closed causal curves) satisfies the first three conditions. It is the local finiteness condition that introduces spacetime discreteness.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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