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Topological Quantum Computing
A Cohomological Framework for Topological Phases from Momentum-Space Crystallographic Groups
arXiv
Authors: T. R. Liu, Zheng Zhang, Y. X. Zhao
Year
2025
Paper ID
36219
Status
Preprint
Abstract Read
~2 min
Abstract Words
238
Citations
N/A
Abstract
Crystallographic groups are conventionally studied in real space to characterize crystal symmetries. Recent work has recognized that when these symmetries are realized projectively, momentum space inherently accommodates nonsymmorphic symmetries, thereby evoking the concept of momentum-space crystallographic groups (MCGs). Here, we reveal that the cohomology of MCGs encodes fundamental data of crystalline topological band structures. Specifically, the collection of second cohomology groups, H2\(ΓF,mathbb{Z}\), for all MCGs ΓF, provides an exhaustive classification of Abelian crystalline topological insulators, serving as an effective approximation to the full crystalline topological classification. Meanwhile, the third cohomology groups H3\(ΓF,mathbb{Z}\) across all MCGs exhaustively classify all possible twistings of point-group actions on the Brillouin torus, essential data for twisted equivariant K-theory. Furthermore, we establish the isomorphism Hn+1\(ΓF,mathbb{Z}\)cong Hnbig\(ΓF,operatorname{mathcal{F}}(mathbb{R}dF,U(1\))big) for nge 1, where operatorname{mathcal{F}}\(mathbb{R}dF,U(1\)) denotes the space of continuous U(1)-valued functions on the dD momentum space mathbb{R}dF. The case n=1 yields a complete set of topological invariants formulated in purely algebraic terms, which differs fundamentally from the conventional formulation in terms of differential forms. The case n=2, analogously, provides a fully algebraic description for all such twistings. Thus, the cohomological theory of MCGs serves as a key technical framework for analyzing crystalline topological phases within the general setting of projective symmetry.
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