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PF:2026.000008 · Mathematical Physics

Covariance of Buchholz--Fredenhagen Categories under QCA, Reflection, and Time Reversal

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  1. Ruizhi Liu · Perimeter Institute
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Definition 1.1: [Def.~1.1

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_\Lambda)_\varepsilon\bigr). \item For every such $\delta$ and every $t\ge0$ there is a unitary $\widetilde U_{\Lambda,\varepsilon,\delta,t} \in\R_\psi(\Lambda_{\varepsilon+\delta}-te_\Lambda)$ with \|U_{\Lambda,\varepsilon}-\widetilde U_{\Lambda,\varepsilon,\delta,t}\| \le f_{\varphi,\varepsilon,\delta}(t).

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  1. D. 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 reference
  2. P. 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}.
    External reference
  3. P. Naaijkens, Localized endomorphisms in Kitaev's toric code on the plane, Rev. Math. Phys. 23 (2011), 347--373. doi:10.1142/S0129055X1100431X; arXiv:1012.3857.
    LaTeX source\bibitem{Naaijkens2011} P.~Naaijkens, \emph{Localized endomorphisms in Kitaev's toric code on the plane}, Rev. Math. Phys. \textbf{23} (2011), 347--373. \href{https://doi.org/10.1142/S0129055X1100431X}{doi:10.1142/S0129055X1100431X}; \href{https://arxiv.org/abs/1012.3857}{arXiv:1012.3857}.
    External reference
  4. Y. 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 reference
  5. Y. 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}.
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  6. S. 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 reference
  7. C. 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 reference
  8. A. 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 reference
  9. P. 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}.
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  10. M. 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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Machine-readable theorem index · 6 statements

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  1. 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…

  2. 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…

  3. 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.

  4. 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 $S$.

  5. 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)'.

  6. 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 $f'$.