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Introduction Quantum Kripke Frames Directions for Future Work On a Connection between Piron Lattices and Kripke Frames Shengyang Zhong (zhongshengyang@163.com) Institute for Logic, Language and Computation, University of Amsterdam November


  1. Introduction Quantum Kripke Frames Directions for Future Work On a Connection between Piron Lattices and Kripke Frames Shengyang Zhong (zhongshengyang@163.com) Institute for Logic, Language and Computation, University of Amsterdam November 30th, 2013 Whither Quantum Structures in the XXIth Century? Brussels, Belgium Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  2. Introduction Quantum Kripke Frames Directions for Future Work Outline Introduction 1 Quantum Kripke Frames 2 Definition and Main Result Relations with Other Structures Probabilistic Quantum Kripke Frames Directions for Future Work 3 Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  3. Introduction Quantum Kripke Frames Directions for Future Work Outline Introduction 1 Quantum Kripke Frames 2 Definition and Main Result Relations with Other Structures Probabilistic Quantum Kripke Frames Directions for Future Work 3 Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  4. Introduction Quantum Kripke Frames Directions for Future Work Orthogonality Relation in Quantum Theory Consider an isolated quantum system described by some Hilbert space H over complex numbers. Two non-zero vectors | ψ � and | φ � are said to be orthogonal, denoted as | ψ � ⊥ | φ � , if the inner product � ψ | φ � is 0. This binary relation on vectors induces a binary relation on one-dimensional subspaces of H and thus on states of the quantum system, which is also called orthogonality relation. By studying this relation, we get many representation theorems for lattices emerging from quantum logic via Kripke frames. Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  5. Introduction Quantum Kripke Frames Directions for Future Work Ortholattices and Orthogonality Spaces [Goldblatt, 1974] ‘That the ⊥ -closed subsets of an orthogonality space form an ortholattice under the partial ordering of set inclusion is a result of long standing (cf. Birkhoff,[1] § V.7).’ ‘Every ortholattice is, within isomorphism, a subortholattice of the lattice of ⊥ -closed subsets of some orthogonality space.’ Ortholattice: an orthocomplemented lattice Orthogonality space: a Kripke frame in which the binary relation is irreflexive and symmetric . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  6. Introduction Quantum Kripke Frames Directions for Future Work Property Lattices and State Spaces [Moore, 1995] Property lattice: a complete atomistic orthocomplemented lattice . State space: a Kripke frame (Σ , ⊥ ) in which the binary relation ⊥ is irreflexive , symmetric and separated in the following sense: there is w ∈ Σ such that w ⊥ s and w �⊥ t, for any s , t ∈ Σ such that s � = t. The main result in this paper is a duality between a category with property lattices as objects, and a category with state spaces as objects. Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  7. Introduction Quantum Kripke Frames Directions for Future Work What about Piron Lattices? Compared to lattices emerging from quantum theory, i.e. lattices of closed linear subspaces of Hilbert spaces, both ortholattices and property lattices are too general. Piron lattice: an irreducible, complete, atomistic, orthocomplemented lattices satisfying weak modularity and the Covering Law . They are also called irreducible propositional systems . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  8. Introduction Quantum Kripke Frames Directions for Future Work Piron Lattices and Hilbert Spaces Piron’s Theorem (1964) The lattice of bi-orthogonally closed subspaces of a generalized Hilbert space is always a Piron lattice; and every Piron lattice of rank at least 4 is isomorphic to such a lattice. A Corollary of the Amemiya-Araki-Piron Theorem Generalized Hilbert spaces over the real numbers, the complex numbers and the quaternions are Hilbert spaces over these ∗ -fields, in such a way that bi-orthogonally closed subspaces are exactly closed linear subspaces. Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  9. Introduction Quantum Kripke Frames Directions for Future Work Piron Lattices and Quantum Dynamic Frames In [Baltag and Smets, 2005], the authors give a representation theorem for Piron lattices (satisfying Mayet’s condition) using quantum dynamic frames . A quantum dynamic frame is a tuple (Σ , { P ? →} P ∈L ), where Σ is a non-empty set, L is a subset of the power set of Σ and P ? → is a binary relation on Σ for all P ∈ L . The orthogonality relation, denoted as ⊥ , is defined as follows: there is no P ∈ L such that s P ? s ⊥ t ⇐ ⇒ → t . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  10. Introduction Quantum Kripke Frames Directions for Future Work The Work in this Talk I will define a kind of Kripke frames, and use them to give a representation theorem for Piron lattices. This work inspired by Baltag and Smets’ work, provides an alternative way of defining quantum dynamic frame; continues the logical study of the orthogonality relation extending Moore’s result and thus Goldblatt’s result. Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  11. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Outline Introduction 1 Quantum Kripke Frames 2 Definition and Main Result Relations with Other Structures Probabilistic Quantum Kripke Frames Directions for Future Work 3 Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  12. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Outline Introduction 1 Quantum Kripke Frames 2 Definition and Main Result Relations with Other Structures Probabilistic Quantum Kripke Frames Directions for Future Work 3 Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  13. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Some Terminologies of Kripke Frames Kripke Frame A Kripke frame F is a tuple (Σ , → ), where Σ is a non-empty set and → ⊆ Σ × Σ. Write s �→ t for ( s , t ) �∈ → . Given P ⊆ Σ, the orthocomplement of P (w.r.t. → ) is defined as follows: ∼ P def = { s ∈ Σ | s �→ t , for every t ∈ P } P is bi-orthogonally closed, if P = ∼∼ P . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  14. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Quantum Kripke Frames Definition (Quantum Kripke Frame) A quantum Kripke frame (QKF) F is a Kripke frame (Σ , → ) satisfying the following conditions: (i) → is reflexive and symmetric. (ii) (Existence of Good Approximation) if s �∈ ∼ P and ∼∼ P = P , then there is t ∈ P such that s → u if and only if t → u for each u ∈ P ; (iii) (Separation) if s � = t , then there is w ∈ Σ such that w → s and w �→ t ; (iv) (Superposition) for any s , t ∈ Σ, there is w ∈ Σ such that w → s and w → t . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  15. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Good Approximations are the Best Consider s ∈ Σ and P ⊆ Σ such that good approximation of s in P exists according to condition (ii). There is t ∈ P such that s → u ⇔ t → u , for every u ∈ P . Condition (iii), i.e. Separation, guarantees that the t with this property is unique. This t will be called the best approxiamtion of s in P . Given a bi-orthogonally closed P ⊆ Σ, define a partial function P ?( · ) : Σ ��� Σ as follows: � the best approxiamtion t of s in P , if s �∈ ∼ P P ?( s ) def = undefined , otherwise Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

  16. Introduction Definition and Main Result Quantum Kripke Frames Relations with Other Structures Directions for Future Work Probabilistic Quantum Kripke Frames Main Results Theorem 1 For any quantum Kripke frame F = (Σ , → ), ( L F , ⊆ , ∼ ( · )) is a Piron lattice, where L F = { P ⊆ Σ | ∼∼ P = P } and ∼ ( · ) is the orthocomplement operation (w.r.t. → ). Theorem 2 Every Piron lattice L is isomorphic to ( L F , ⊆ , ∼ ( · )) for some quantum Kripke frame F . Shengyang Zhong (zhongshengyang@163.com) On a Connection between Piron Lattices and Kripke Frames

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