Abstract
Despite the plausible necessity of topological protection for realizing scalable quantum computers, the conceptual underpinnings of topological quantum logic gates had arguably remained shaky, both regarding their physical realization as well as their information-theoretic nature. Building on recent results on defect branes in string/M-theory (Sati and Schreiber in Rev Math Phys, 2023. https://doi.org/10.1142/S0129055X23500095. [ar**v:2203.11838]) and on their holographically dual anyonic defects in condensed matter theory (Sati and Schreiber in Rev Math Phys 35(03):2350001, 2023. https://doi.org/10.1142/S0129055X23500010. [ar**v:2206.13563]), here we explain [as announced in Sati and Schreiber (PlanQC 2022:33, 2022, [ar**v:2209.08331], [ncatlab.org/schreiber/show/Topological+Quantum+Programming+in+TED-K])] how the specification of realistic topological quantum gates, operating by anyon defect braiding in topologically ordered quantum materials, has a surprisingly slick formulation in parameterized point-set topology, which is so fundamental that it lends itself to certification in modern homotopically typed programming languages, such as cubical Agda. We propose that this remarkable confluence of concepts may jointly kickstart the development of topological quantum programming proper as well as of real-world application of homotopy type theory, both of which have arguably been falling behind their high expectations; in any case, it provides a powerful paradigm for simulating and verifying topological quantum computing architectures with high-level certification languages aware of the actual physical principles of realistic topological quantum hardware. In companion articles (Sati and Schreiber in The Quantum Monadology, [ar**v:2310.15735], Sati and Schreiber in Entanglement of Sections: The pushout of entangled and parameterized quantum information [ar**v:2309.07245]) [announced in Schreiber (Quantum types via Linear Homotopy Type Theory, talk at Workshop on Quantum Software @ QTML2022, Naples, 2022, [ncatlab.org/schreiber/files/QuantumDataInLHoTT-221117.pdf])], we explain how further passage to “dependent linear” homotopy types naturally extends this scheme to a full-blown quantum programming/certification language in which our topological quantum gates may be compiled to verified quantum circuits, complete with quantum measurement gates and classical control.
Notes
Intriguingly, cohesive linear homotopy theory is also the semantic context in which to naturally make formal sense of the key ingredients of high energy physics, specifically of string/M-theory (cf. [Sc14b][
As is usual, in (60) we are including denotation of a generic context of “constants” c of any type \(\Gamma \) – on which the execution of f may well depend, but which one may not want to regard as external parameters but as implicit arguments passed to the program (e.g. “flags”). As also usual, often we will notationally suppress this generic background context.
The traditional notation for the dependent pair type is some variant of “\(\sum _{d \,:\, D} C_d\)”, pronounced the “dependent sum”. While widely used, this is clearly a misnomer—and it becomes a fatal misnomer once we generalize dependent type theory to dependent linear type theory [147), following [; alternatively one could rewrite these definitions to regard it as extra structure on . The distinction, which traditional literature glosses over anyway, is a matter of convention rather than of practical content.
The inclusion (208) is of course a homomorphism of monoid (semi-group) data structures, but here we do not dwell on monoid structure, for brevity.
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Communicated by A. Childs.
In Memoriam of Yuri Manin who introduced quantum computation as well as Gauss-Manin connections unknowing of their close relationship.
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Myers, D.J., Sati, H. & Schreiber, U. Topological Quantum Gates in Homotopy Type Theory. Commun. Math. Phys. 405, 172 (2024). https://doi.org/10.1007/s00220-024-05020-8
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DOI: https://doi.org/10.1007/s00220-024-05020-8