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arXiv:1806.02840 · Communications in Mathematical Physics

Contextuality and Noncommutative Geometry in Quantum Mechanics

Nadish de Silva, Rui Soares Barbosa

Published Jan 1, 2019• 8 citations
arXivHTMLPDF

Abstract

Observable properties of a classical physical system can be modelled deterministically as functions from the space of pure states to outcome values; dually, states can be modelled as functions from the algebra of observables to outcome values. The probabilistic predictions of quantum physics are contextual in that they preclude this classical assumption of reality: noncommuting observables, which are not assumed to be jointly measurable, cannot be consistently ascribed deterministic values even if one enriches the description of a quantum state. Here, we consider the geometrically dual objects of noncommutative operator algebras of observables as being generalisations of classical (deterministic) state spaces to the quantum setting and argue that these generalised state spaces represent the objects of study of noncommutative operator geometry. By adapting the spectral presheaf of Hamilton–Isham–Butterfield, a formulation of quantum state space that collates contextual data, we reconstruct tools of noncommutative geometry in an explicitly geometric fashion. In this way, we bridge the foundations of quantum mechanics with the foundations of noncommutative geometry à la Connes et al. To each unital C*- algebra $${\mathcal{A}}$$ we associate a geometric object—a diagram of topological spaces collating quotient spaces of the noncommutative space underlying $${\mathcal{A}}$$ —that performs the role of a generalised Gel'fand spectrum. We show how any functor F from compact Hausdorff spaces to a suitable target category $${\mathsf{C}}$$ can be applied directly to these geometric objects to automatically yield an extension $${\tilde{F}}$$ acting on all unital C*-algebras. This procedure is used to give a novel formulation of the operator K0-functor via a finitary variant $${\tilde{K}_{ f}}$$ of the extension $${\tilde{K}}$$ of the topological K-functor. We then delineate a C*-algebraic conjecture that the extension of the functor that assigns to a topological space its lattice of open sets assigns to a unital C*-algebra the Zariski topological lattice of its primitive ideal spectrum, i.e. its lattice of closed two-sided ideals. We prove the von Neumann algebraic analogue of this conjecture.

DOI
10.1007/s00220-018-3222-9

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Observable properties of a classical physical system can be modelled deterministically as functions from the space of pure states to outcome values; dually, states can be modelled as functions from the algebra of observables to outcome values. The probabilistic predictions of quantum physics are contextual in that they preclude this classical assumption of reality: noncommuting observables, which are not assumed to be jointly measurable, cannot be consistently ascribed deterministic values even if one enriches the description of a quantum state. Here, we consider the geometrically dual objects of noncommutative operator algebras of observables as being generalisations of classical (deterministic) state spaces to the quantum setting and argue that these generalised state spaces represent the objects of study of noncommutative operator geometry. By adapting the spectral presheaf of Hamilton–Isham–Butterfield, a formulation of quantum state space that collates contextual data, we reconstruct tools of noncommutative geometry in an explicitly geometric fashion. In this way, we bridge the foundations of quantum mechanics with the foundations of noncommutative geometry à la Connes et al. To each unital C*- algebra A{\mathcal{A}}A we associate a geometric object—a diagram of topological spaces collating quotient spaces of the noncommutative space underlying A{\mathcal{A}}A —that performs the role of a generalised Gel'fand spectrum. We show how any functor F from compact Hausdorff spaces to a suitable target category C{\mathsf{C}}C can be applied directly to these geometric objects to automatically yield an extension F~{\tilde{F}}F~ acting on all unital C*-algebras. This procedure is used to give a novel formulation of the operator K0-functor via a finitary variant K~f{\tilde{K}_{ f}}K~f​ of the extension K~{\tilde{K}}K~ of the topological K-functor. We then delineate a C*-algebraic conjecture that the extension of the functor that assigns to a topological space its lattice of open sets assigns to a unital C*-algebra the Zariski topological lattice of its primitive ideal spectrum, i.e. its lattice of closed two-sided ideals. We prove the von Neumann algebraic analogue of this conjecture.
The aim of this paper is to relate algebraic quantum mechanics to topos theory, so as to construct new foundations for quantum logic and quantum spaces. Motivated by Bohr’s idea that the empirical content of quantum physics is accessible only through classical physics, we show how a noncommutative C*-algebra of observables A induces a topos T(A){\mathcal{T}(A)}T(A) in which the amalgamation of all of its commutative subalgebras comprises a single commutative C*-algebra A‾{\underline{A}}A​ . According to the constructive Gelfand duality theorem of Banaschewski and Mulvey, the latter has an internal spectrum Σ‾(A‾){\underline{\Sigma}(\underline{A})}Σ​(A​) in T(A){\mathcal{T}(A)}T(A) , which in our approach plays the role of the quantum phase space of the system. Thus we associate a locale (which is the topos-theoretical notion of a space and which intrinsically carries the intuitionistic logical structure of a Heyting algebra) to a C*-algebra (which is the noncommutative notion of a space). In this setting, states on A become probability measures (more precisely, valuations) on Σ‾{\underline{\Sigma}}Σ​ , and self-adjoint elements of A define continuous functions (more precisely, locale maps) from Σ‾{\underline{\Sigma}}Σ​ to Scott’s interval domain. Noting that open subsets of Σ‾(A‾){\underline{\Sigma}(\underline{A})}Σ​(A​) correspond to propositions about the system, the pairing map that assigns a (generalized) truth value to a state and a proposition assumes an extremely simple categorical form. Formulated in this way, the quantum theory defined by A is essentially turned into a classical theory, internal to the topos T(A){\mathcal{T}(A)}T(A) .These results were inspired by the topos-theoretic approach to quantum physics proposed by Butterfield and Isham, as recently generalized by Döring and Isham.
In the topos approach to quantum theory of Doering and Isham the Kochen-Specker Theorem, which asserts the contextual nature of quantum theory, can be reformulated in terms of the global sections of a presheaf characterised by the Gelfand spectrum of a commutative C*-algebra. In previous work we showed how this topos perspective can be generalised to a class of categories typically studied within the monoidal approach to quantum theory of Abramsky and Coecke, and in particular how one can generalise the Gelfand spectrum. Here we study the Gelfand spectrum presheaf for categories of quantale-valued relations, and by considering its global sections we give a non-contextuality result for these categories. We also show that the Gelfand spectrum comes equipped with a topology which has a natural interpretation when thinking of these structures as representing physical theories.
We study the mathematical structure of the notion of measurement space, which extends aspects of noncommutative topology that are based on quantale theory. This yields a geometric model of physical measurements that provides a realist picture, yet also operational, such that measurements and classical information arise interdependently as primitive concepts. A derived notion of classical observer caters for a mathematical formulation of Bohr's classical/quantum divide. Two important classes of measurement spaces are obtained, respectively from C*-algebras and from second-countable locally compact open sober topological groupoids. The latter yield measurements of classical type and relate to Schwinger's notion of selective measurement. We show that the measurement space associated to the reduced C*-algebra of any second-countable locally compact Hausdorff étale groupoid is canonically equipped with a classical observer, and we establish a correspondence between properties of the observer and properties of the groupoid.
Classical Gelfand duality provides an equivalence between commutative C-star algebras and topological spaces, but fails to furnish a geometric object for noncommutative operator systems. To address this, we introduce a categorified notion of spectrum that captures the full operator-semantic structure. For an operator system A, we construct a spectral stack, denoted Spec(A), over the site of its commutative contexts. The construction proceeds in three stages. First, we encode the syntax of A via a colored operad called the synergy operad. Second, we aggregate local semantic data using a left Kan extension, providing an explicit coend formula. Third, we enforce descent via sheafification, yielding a stack that satisfies higher gluing conditions. We prove that Spec(A) satisfies a Yoneda-style universal property, making it the initial descent-complete semantic realization of A. This yields a contravariant functor from operator systems to spectral objects that admits a right adjoint, the global sections functor. Under semantic generation and descent completeness, the counit of this adjunction is an equivalence, establishing a reconstruction theorem: A is isomorphic to the endomorphisms of the structure sheaf on its spectrum. We further provide a recognition theorem characterizing the essential image of this functor and prove Morita invariance of the associated quasi-coherent sheaf categories. The construction naturally recovers classical Gelfand spectra and Bohrification as truncations of a Postnikov tower. Explicit computations for matrix algebras, Pauli systems, and the Mermin-Peres square yield a quantitative invariant of contextuality extracted from the inertia stack of Spec(A). Comparison theorems show that our framework subsumes Gelfand duality, Bohrification, and Tannaka reconstruction as special cases.
Quantum mechanics fundamentally challenges classical intuitions regarding reality and measurement, most notably through contextuality theorems such as Kochen-Specker and Bell-type inequalities. Traditional formulations treat measurement contexts as discrete sets of compatible observables or operational setups without a native, continuous geometric topology. In this paper, we introduce the framework of Quantum Measurement Context Curvature (QMCC), proposing that sequential, non-commutative measurements and environments naturally induce an irreducible geometric structure known as context curvature. By defining measurement contexts as ordered tuples C = (M_1, M_2, ..., M_n) and constructing non-commutative loops in context space, we quantify the path-dependence of quantum transition probabilities. We formalize the context curvature R_C as a sum over loops involving conditional probability discrepancies between alternative measurement orderings. This geometric perspective transcends standard operational descriptions, establishing a formal bridge between non-commutative algebraic structures of quantum mechanics and differential geometry, with potential applications in foundational quantum mechanics and advanced quantum information processing.
This paper establishes the theoretical framework of Observer Algebraic Geometry, modeling the observer as a coherent sheaf structure on a noncommutative algebraic variety. Based on the area spectrum of loop quantum gravity and the spectraltriple of noncommutative geometry, we prove that the algebraic dimension of theminimal observer unit is approximately 62.5, a value determined by the BarberoImmirzi parameter. Within this framework, the observation act is reinterpreted asa mirror equivalence between the derived category and the Fukaya category, andthe observation backreaction is described by a nonlocal operator whose algebraicstructure leads to a fundamental bound on the cognitive-physical uncertainty. Thetheory predicts an observer horizon at the Planck scale, a sheaf cohomology criterion for the emergence of consciousness in AI systems, and characteristic oscillationmodes in the cosmic microwave background radiation. This framework incorporatesthe observer into the geometrization program, providing a rigorous mathematicalformulation for the quantum measurement problem.