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arXiv:0803.0417 · Lecture notes in physics

“What is a Thing?”: Topos Theory in the Foundations of Physics

A. Döring, C. Isham

Published Jan 1, 2010• 127 citations
arXivHTMLPDF
DOI
10.1007/978-3-642-12821-9_13

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A topos foundation for theories of physics: III. The representation of physical quantities with arrows δo(A):Σ→R≽

Andreas Döring, Christopher John Isham

This paper is the third in a series whose goal is to develop a fundamentally new way of viewing theories of physics. Our basic contention is that constructing a theory of physics is equivalent to finding a representation in a topos of a certain formal language that is attached to the system. In Paper II, we studied the topos representations of the propositional language PL(S) for the case of quantum theory, and in the present paper we do the same thing for the, more extensive, local language L(S). One of the main achievements is to find a topos representation for self-adjoint operators. This involves showing that, for any physical quantity A, there is an arrow δ̆o(A):Σ̱→R≽̱, where R≽̱ is the quantity-value object for this theory. The construction of δ̆o(Â) is an extension of the daseinisation of projection operators that was discussed in Paper II. The object R≽̱ is a monoid object only in the topos, τϕ=SetsV(H)op, of the theory, and to enhance the applicability of the formalism, we apply to R≽̱ a topos analog of the Grothendieck extension of a monoid to a group. The resulting object, k(R≽̱), is an abelian group object in τϕ. We also discuss another candidate, R↔̱, for the quantity-value object. In this presheaf, both inner and outer daseinisations are used in a symmetric way. Finally, there is a brief discussion of the role of unitary operators in the quantum topos scheme.

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A topos foundation for theories of physics: IV. Categories of systems

Andreas Döring, Christopher John Isham

This paper is the fourth in a series whose goal is to develop a fundamentally new way of building theories of physics. The motivation comes from a desire to address certain deep issues that arise in the quantum theory of gravity. Our basic contention is that constructing a theory of physics is equivalent to finding a representation in a topos of a certain formal language that is attached to the system. Classical physics arises when the topos is the category of sets. Other types of theory employ a different topos. The previous papers in this series are concerned with implementing this program for a single system. In the present paper, we turn to considering a collection of systems; in particular, we are interested in the relation between the topos representation for a composite system and the representations for its constituents. We also study this problem for the disjoint sum of two systems. Our approach to these matters is to construct a category of systems and to find a topos representation of the entire category.

arXiv:quant-ph/0703066•Journal of Mathematical Physics•May 1, 2008•87 citations
This paper is the third in a series whose goal is to develop a fundamentally new way of viewing theories of physics. Our basic contention is that constructing a theory of physics is equivalent to finding a representation in a topos of a certain formal language that is attached to the system. In Paper II, we studied the topos representations of the propositional language PL(S) for the case of quantum theory, and in the present paper we do the same thing for the, more extensive, local language L(S). One of the main achievements is to find a topos representation for self-adjoint operators. This involves showing that, for any physical quantity A, there is an arrow δ̆o(A):Σ̱→R≽̱, where R≽̱ is the quantity-value object for this theory. The construction of δ̆o(Â) is an extension of the daseinisation of projection operators that was discussed in Paper II. The object R≽̱ is a monoid object only in the topos, τϕ=SetsV(H)op, of the theory, and to enhance the applicability of the formalism, we apply to R≽̱ a topos analog of the Grothendieck extension of a monoid to a group. The resulting object, k(R≽̱), is an abelian group object in τϕ. We also discuss another candidate, R↔̱, for the quantity-value object. In this presheaf, both inner and outer daseinisations are used in a symmetric way. Finally, there is a brief discussion of the role of unitary operators in the quantum topos scheme.
This paper is the fourth in a series whose goal is to develop a fundamentally new way of building theories of physics. The motivation comes from a desire to address certain deep issues that arise in the quantum theory of gravity. Our basic contention is that constructing a theory of physics is equivalent to finding a representation in a topos of a certain formal language that is attached to the system. Classical physics arises when the topos is the category of sets. Other types of theory employ a different topos. The previous papers in this series are concerned with implementing this program for a single system. In the present paper, we turn to considering a collection of systems; in particular, we are interested in the relation between the topos representation for a composite system and the representations for its constituents. We also study this problem for the disjoint sum of two systems. Our approach to these matters is to construct a category of systems and to find a topos representation of the entire category.