ar X iv : 1 50 4 . 00 51 2 v 1 [ cs . L O ] 2 A pr 2 01 5 Dynamic Causality in Event Structures ( Technical Report )
نویسندگان
چکیده
In [1] we present an extension of Prime Event Structures by a mechanism to express dynamicity in the causal relation. More precisely we add the possibility that the occurrence of an event can add or remove causal dependencies between events and analyse the expressive power of the resulting Event Structures w.r.t. to some well-known Event Structures from the literature. This technical report contains some additional information and the missing proofs of [1]. 1 Event Structures for Resolvable Conflict For a transition based ES with a few additional properties, there is a natural embedding into RCESs. Definition 20. Let μ be an ES with a transition relation → defined on configurations such that X → Y implies X ⊆ Y and X ⊆ X ′ ⊆ Y ′ ⊆ Y implies that X → Y =⇒ X ′ → Y ′ for all configurations X,Y,X , Y ′ of μ. Then rces(μ) = (E, {X ⊢ Z | ∃Y ⊆ E . X→Y ∧ Z ⊆ Y }). Note that the SESs and GESs satisfy these properties. We show that the resulting structure rces(μ) is indeed an RCES and that it is transition equivalent to μ. Lemma 2. Let μ be an ES that satisfies the conditions of Def. 20. Then rces(μ) is a RCES and rces(μ)≃tμ. Proof. By Def. 9 in [1], rces(μ) is a RCES. Assume X→Y . Then, by Def. 20, X ⊆ Y and X ⊢ Z for all Z ⊆ Y .Then, by Def. 10 in [1], X→rcY . Assume X→rcY . Then, by Def. 10 in [1], X ⊆ Y and there is some X ′ ⊆ X such that X ′ ⊢ Y . By Def. 20 for rces(·), then X ′ ⊢ Y ′ for all Y ′ ⊆ Y . So there is a set Ỹ such that Y ⊆ Ỹ and X ′ ⊢ Ỹ ′ for each Ỹ ′ ⊆ Ỹ . Then, by Def. 20 for rces(·), it follows X ′ → Ỹ ′ and X ′ ⊆ X ⊆ Y ⊆ Ỹ . Finally, by the second property of Def. 20, X→Y . ⋆ Supported by the DFG Research Training Group SOAMED. 2 Youssef Arbach, David Karcher, Kirstin Peters, Uwe Nestmann
منابع مشابه
ar X iv : g r - qc / 0 51 01 27 v 1 3 1 O ct 2 00 5 Imprints of Spacetime Topology in the Hawking - Unruh Effect
متن کامل
ar X iv : 1 30 4 . 51 85 v 2 [ cs . L O ] 3 0 A pr 2 01 3 Temporal Description Logic for Ontology - Based Data Access ( Extended
Our aim is to investigate ontology-based data access over temporal data with validity time and ontologies capable of temporal conceptual modelling. To this end, we design a temporal description logic, TQL, that extends the standard ontology language OWL 2 QL, provides basic means for temporal conceptual modelling and ensures first-order rewritability of conjunctive queries for suitably defined ...
متن کامل. pl as m - p h ] 1 4 M ay 2 00 5 Two - fluid tokamak equilibria with reversed magnetic shear and sheared flow 1
X iv :p hy si cs /0 50 51 01 v1 [ ph ys ic s. pl as m -p h] 1 4 M ay 2 00 5 Two-fluid tokamak equilibria with reversed magnetic shear and sheared flow 1 G. Poulipoulis, G. N. Throumoulopoulos, H. Tasso University of Ioannina, Association Euratom Hellenic Republic, Section of Theoretical Physics, GR 451 10 Ioannina, Greece Max-Planck-Institut für Plasmaphysik, Euratom Association, D-85748 Garchi...
متن کاملar X iv : h ep - p h / 03 04 01 2 v 1 1 A pr 2 00 3 CHAPTER 1 EVENT BY EVENT FLUCTUATIONS
Contents 1. Introduction 3 2. Fluctuations in a thermal system 6 2.1. Fluctuations in a grand canonical ensemble 6 2.1.1. Fluctuations of the energy and of the conserved charges 7 2.2. Fluctuations in a canonical ensemble 11 2.3. Phase Transitions and Fluctuations 13 3. Other fluctuations 15 3.1. Volume fluctuations 15 3.2. Fluctuation from initial collisions 17 4. Fluctuations and Correlations...
متن کامل