Covariance of Buchholz--Fredenhagen Categories under QCA, Reflection, and Time Reversal
Let $\psi$ be a pure state of a two-dimensional quantum spin system, and assume that its GNS representation satisfies approximate Haag duality (AHD) in the sense of Ogata. Using product-state stabilization to make the cone von Neumann algebras properly infinite, the cone sectors of $\psi$ form a braided Buchholz--Fredenhagen (BF) $C^*$-tensor category $\operatorname{BF}(\psi)$. We show how $\operatorname{BF}(\psi)$ changes under three operations. (i) A quantum cellular automaton (QCA) of finite spread preserves AHD and gives a linear braided equivalence. (ii) A spatial reflection gives a linear equivalence that reverses the braiding. (iii) An on-site time reversal gives an anti-linear braided equivalence; in other words, the complex conjugate of $\operatorname{BF}(\psi)$ is braided equivalent to the BF category of the time-reversed state. For QCA we give a direct proof that AHD is preserved, with explicit constants. We also compare the QCA result with related results of Ogata, Naaijkens--Ogata, Jones, and Bhardwaj--Brisky--Chuah--Kawagoe--Keslin--Penneys--Wallick.
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Proposition 4.2
If $\psi$ satisfies AHD as in Definition 1.1 and $\alpha$ satisfies the spread condition (equation reference) of Theorem 2.1(i), then $\psi_\alpha$ satisfies AHD with R'_{\varphi,\varepsilon} &:=\kappa_R(\varphi)+R_{\varphi,\varepsilon}+\kappa_R(\varphi+2\varepsilon), \\ f'_{\varphi,\varepsilon,\delta}(t) &:= 2, & 0\le t<C,\\ f_{\varphi,\varepsilon,\delta}(t-C), & t\ge C, \qquad C:=\kappa_R(\varphi)+\kappa_R(\varphi+2\varepsilon+2\delta). In particular, if the functions $f$ for $\psi$ decay exponentially (or faster than any power), so do the functions $f'$.
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- External referenceD. Buchholz and K. Fredenhagen, Locality and the structure of particle states, Commun. Math. Phys. 84 (1982), 1--54. doi:10.1007/BF01208370.LaTeX source\bibitem{BuchholzFredenhagen1982} D.~Buchholz and K.~Fredenhagen, \emph{Locality and the structure of particle states}, Commun. Math. Phys. \textbf{84} (1982), 1--54. \href{https://doi.org/10.1007/BF01208370}{doi:10.1007/BF01208370}.
- External referenceP. Naaijkens, On the extension of stringlike localised sectors in $2+1$ dimensions, Commun. Math. Phys. 303 (2011), 385--420. doi:10.1007/s00220-011-1200-6.LaTeX source\bibitem{NaaijkensBF2011} P.~Naaijkens, \emph{On the extension of stringlike localised sectors in $2+1$ dimensions}, Commun. Math. Phys. \textbf{303} (2011), 385--420. \href{https://doi.org/10.1007/s00220-011-1200-6}{doi:10.1007/s00220-011-1200-6}.
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- External referenceY. Ogata, A derivation of braided $C^*$-tensor categories from gapped ground states satisfying the approximate Haag duality, J. Math. Phys. 63 (2022), 011902. doi:10.1063/5.0061785; arXiv:2106.15741.LaTeX source\bibitem{Ogata2022} Y.~Ogata, \emph{A derivation of braided $C^*$-tensor categories from gapped ground states satisfying the approximate Haag duality}, J. Math. Phys. \textbf{63} (2022), 011902. \href{https://doi.org/10.1063/5.0061785}{doi:10.1063/5.0061785}; \href{https://arxiv.org/abs/2106.15741}{arXiv:2106.15741}.
- External referenceY. Ogata, Mixed state topological order: operator algebraic approach, arXiv:2501.02398 [math-ph] (2025). arXiv:2501.02398.LaTeX source\bibitem{Ogata2025Mixed} Y.~Ogata, \emph{Mixed state topological order: operator algebraic approach}, arXiv:2501.02398 [math-ph] (2025). \href{https://arxiv.org/abs/2501.02398}{arXiv:2501.02398}.
- External referenceS. Bachmann, A. Getz, P. Naaijkens, and N. Wray, Stacking and the triviality of invertible phases, arXiv:2511.08382 [math-ph] (2026). arXiv:2511.08382.LaTeX source\bibitem{bachmann2026stackingtrivialityinvertiblephases} S.~Bachmann, A.~Getz, P.~Naaijkens, and N.~Wray, \emph{Stacking and the triviality of invertible phases}, arXiv:2511.08382 [math-ph] (2026). \href{https://arxiv.org/abs/2511.08382}{arXiv:2511.08382}.
- External referenceC. Jones, DHR bimodules of quasi-local algebras and symmetric quantum cellular automata, Quantum Topol. 15 (2024), 633--686. doi:10.4171/QT/216; arXiv:2304.00068.LaTeX source\bibitem{Jones2024} C.~Jones, \emph{DHR bimodules of quasi-local algebras and symmetric quantum cellular automata}, Quantum Topol. \textbf{15} (2024), 633--686. \href{https://doi.org/10.4171/QT/216}{doi:10.4171/QT/216}; \href{https://arxiv.org/abs/2304.00068}{arXiv:2304.00068}.
- External referenceA. Bhardwaj, T. Brisky, C. Y. Chuah, K. Kawagoe, J. Keslin, D. Penneys, and D. Wallick, Superselection sectors for posets of von Neumann algebras, Commun. Math. Phys. 406 (2025), Article 185. doi:10.1007/s00220-025-05315-4; arXiv:2410.21454.LaTeX source\bibitem{BBC_KKPW2025} A.~Bhardwaj, T.~Brisky, C.~Y.~Chuah, K.~Kawagoe, J.~Keslin, D.~Penneys, and D.~Wallick, \emph{Superselection sectors for posets of von Neumann algebras}, Commun. Math. Phys. \textbf{406} (2025), Article 185. \href{https://doi.org/10.1007/s00220-025-05315-4}{doi:10.1007/s00220-025-05315-4}; \href{https://arxiv.org/abs/2410.21454}{arXiv:2410.21454}.
- External referenceP. Naaijkens and Y. Ogata, The split and approximate split property in 2D systems: stability and absence of superselection sectors, Commun. Math. Phys. 392 (2022), 921--950. doi:10.1007/s00220-022-04356-3; arXiv:2102.07707.LaTeX source\bibitem{NaaijkensOgata2022} P.~Naaijkens and Y.~Ogata, \emph{The split and approximate split property in 2D systems: stability and absence of superselection sectors}, Commun. Math. Phys. \textbf{392} (2022), 921--950. \href{https://doi.org/10.1007/s00220-022-04356-3}{doi:10.1007/s00220-022-04356-3}; \href{https://arxiv.org/abs/2102.07707}{arXiv:2102.07707}.
- External referenceM. Barkeshli, P. Bonderson, M. Cheng, and Z. Wang, Symmetry fractionalization, defects, and gauging of topological phases, Phys. Rev. B 100 (2019), 115147. doi:10.1103/PhysRevB.100.115147.LaTeX source\bibitem{BBCW2019} M.~Barkeshli, P.~Bonderson, M.~Cheng, and Z.~Wang, \emph{Symmetry fractionalization, defects, and gauging of topological phases}, Phys. Rev. B \textbf{100} (2019), 115147. \href{https://doi.org/10.1103/PhysRevB.100.115147}{doi:10.1103/PhysRevB.100.115147}.
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- PF:2026.000008/v1/DEF-1.1
{Ogata2022}}] A pure state $\psi$ satisfies \emph{approximate Haag duality} (AHD) if the following holds. For all $\varphi\in(0,2\pi)$ and $\varepsilon>0$ with $\varphi+4\varepsilon<2\pi$, there are a constant $R_{\varphi,\varepsilon}\ge0$ and, for each $\delta>0$ with $\varphi+2\varepsilon+2\delta<2\pi$, a decreasing function $f_{\varphi,\varepsilon,\delta}:[0,\infty)\to[0,\infty)$ with $f_{\varphi,\varepsilon,\delta}(t)\to0$ as $t\to\infty$, such that every cone $\Lambda$ with opening angle $\varphi$ has the two properties below. \item There is a unitary $U_{\Lambda,\varepsilon}$ on $\Hil_\psi$ with \R_\psi(\Lambda^c)' \subset \Ad(U_{\Lambda,\varepsilon})\, \R_\psi\bigl((\Lambda-R_{\varphi,\varepsilon}e_\L…
- PF:2026.000008/v1/THM-2.1
Let $\psi$ be a pure state that satisfies AHD as in Definition 1.1. \item \textbf{QCA.} Let $\alpha\in\operatorname{Aut}(\A)$ and $R\ge0$ with \alpha^{\pm1}(\A_X)\subset\A_{X^{+R}} \qquad\text{for all finite }X\subset\Gamma. Then $\psi_\alpha:=\psi\circ\alpha$ is a pure state that satisfies AHD, and \[ F_\alpha(\rho):=\rho\circ\alpha, \qquad F_\alpha(x):=x \] is a unitary braided tensor equivalence $F_\alpha:\BF(\psi)\to\BF(\psi_\alpha)$. Here $\BF(\psi_\alpha)$ is built from the GNS representation $\pi_\psi\circ\alpha$ on $\Hil_\psi$. \item \textbf{Reflection.} Let $r$ be an affine reflection of $\mathbb R^2$ with $r\Gamma=\Gamma$, and let $\beta_r\in\operatorname{Aut}(\A)$ satisfy $\beta_r(\A_X)=\A_{rX}$ f…
- PF:2026.000008/v1/LEM-3.1
Let $\Lambda$ be a cone with opening angle $\varphi\in(0,2\pi)$, let $R\ge0$, and put \[ \kappa_R(\varphi):=\frac{R}{\sin(\varphi/2)}. \] Then \Lambda^{+R}\subset\Lambda-\kappa_R(\varphi)e_\Lambda \qquad\text{and}\qquad \bigl(\Lambda+\kappa_R(\varphi)e_\Lambda\bigr)^{+R}\subset\Lambda.
- PF:2026.000008/v1/LEM-3.2
Let $\alpha$ satisfy the spread condition (equation reference) of Theorem 2.1(i), and let $K,S\subset\mathbb R^2$. If $K^{+R}\subset S$, then $\alpha^{\pm1}(\A_K)\subset\A_S$. In particular, $\alpha^{\pm1}(\A_{(S^{+R})^c})\subset\A_{S^c}$ for every $S$.
- PF:2026.000008/v1/COR-4.1
Under the spread condition (equation reference), Lemmas 3.1 and 3.2 imply that, for every cone $\Lambda$, \alpha^{\pm1}(\A_{\Lambda^c})\subset\A_{(\Lambda+\kappa_\Lambda e_\Lambda)^c}, \\ \R_{\psi_\alpha}(\Lambda)\subset\R_\psi(\Lambda-\kappa_\Lambda e_\Lambda), \qquad \R_\psi(\Lambda)\subset\R_{\psi_\alpha}(\Lambda-\kappa_\Lambda e_\Lambda), \\ \R_\psi\bigl((\Lambda+\kappa_\Lambda e_\Lambda)^c\bigr)' \subset\R_{\psi_\alpha}(\Lambda^c)' \subset\R_\psi\bigl((\Lambda-\kappa_\Lambda e_\Lambda)^c\bigr)'.
- PF:2026.000008/v1/PROP-4.2
If $\psi$ satisfies AHD as in Definition 1.1 and $\alpha$ satisfies the spread condition (equation reference) of Theorem 2.1(i), then $\psi_\alpha$ satisfies AHD with R'_{\varphi,\varepsilon} &:=\kappa_R(\varphi)+R_{\varphi,\varepsilon}+\kappa_R(\varphi+2\varepsilon), \\ f'_{\varphi,\varepsilon,\delta}(t) &:= 2, & 0\le t<C,\\ f_{\varphi,\varepsilon,\delta}(t-C), & t\ge C, \qquad C:=\kappa_R(\varphi)+\kappa_R(\varphi+2\varepsilon+2\delta). In particular, if the functions $f$ for $\psi$ decay exponentially (or faster than any power), so do the functions $f'$.