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Topological invariants of non-Hermitian topological systems can be captured by local topological markers defined on the biorthogonal basis. However, unlike the scenario of Hermitian systems, the dynamics of non-Hermitian local topological marker has not yet received much attention so far. Here in this work, we study the dynamic features of local topological markers in non-Hermitian topological systems. In particular, we focus on the propagation of non-Hermitian topological markers in quench dynamics. We find that for the dynamics with topologically distinct pre- and post-quench Hamiltonians, a flow of local topological markers emerges in the bulk, with its propagation speed related to the maximum group velocity. Taking three different non-Hermitian topological models for example, we numerically calculate the propagation speed, and demonstrate that a simple universal relation between the propagation speed and group velocity does not exist, which is unlike the scenarios in previously studied Hermitian systems. Our results reveal the complexity of the local-topological-marker dynamics in non-Hermitian settings, and would stimulate further study on the matter. -
Keywords:
- non-Hermitian topology /
- quench dynamics /
- open systems
[1] Ashida Y, Gong Z, Ueda M 2020 Adv. Phys. 69 249
Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
[6] El-Ganainy R, Makris K G, Khajavikhan M, Musslimani Z H, Rotter S, Christodoulides D N 2017 Nat. Phys. 14 11
Google Scholar
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Google Scholar
[10] Yao S Y, Song F, Wang Z 2018 Phys. Rev. Lett. 121 136802
Google Scholar
[11] Lee C H, Thomale R 2019 Phy. Rev. B 99 201103
Google Scholar
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Google Scholar
[16] Okuma N, Kawabata K, Shiozaki K, Sato M 2020 Phys. Rev. Lett. 124 086801
Google Scholar
[17] Lee T E 2016 Phy. Rev. Lett. 16 133903
Google Scholar
[18] Zhang X Z, Gong J B, 2020 Phy. Rev. B 101 045415
Google Scholar
[19] Zeng Q B, Yang Y B, Xu Y 2020 Phy. Rev. B 101 020201
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[20] Wang X R, Guo C X, Kou S P 2020 Phy. Rev. B 101 121116
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[21] Li T Y, Zhang Y S, Yi W 2021 Chin. Phys. Lett. 38 030301
Google Scholar
[22] Helbig T, Hofmann T, Imhof S, Abdelghany M, Kiessling T, Molenkamp L W, Lee C H, Szameit A, Greiter M, Thomale R 2020 Nat. Phys. 16 747
Google Scholar
[23] Xiao L, Deng T S, Wang K K, Zhu G, Wang Z, Yi W, Xue P 2020 Nat. Phys. 16 761
Google Scholar
[24] Ghatak A, Brandenbourger M, van Wezel J, Coulais C 2020 Proc. Natl. Acad. Sci. U.S.A. 117 29561
Google Scholar
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Google Scholar
[26] Longhi S 2019 Phys. Rev. Res. 1 023013
Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
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Google Scholar
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图 1 非厄米局域拓扑指标的标度行为. 系统中心的非厄米局域拓扑指标随着
$m$ 的变化遵循$(m-m_{\rm c})L^{\tfrac{1}{\nu}}$ 的标度行为. 在$L$ 分别取$15, 17, 19, 21, 23, 25, 27$ 等值时(对应于图中不同颜色的曲线), 所有曲线经变换后遵循同一函数形式, 经拟合得到$\nu\approx 1.1259$ . 在本文的数值计算中, 取$t_1=1$ ,$\gamma_x=\gamma_y=0.3$ Figure 1. Scaling behavior of the non-Hermitian local topological marker near the topological phase transition. The numerically calculated local topological markers for different system sizes (
$L=15, 17, 19, 21, 23, 25, 27$ ) collapse to the same curve, with the functional form$(m-m_{\rm c})L^{\tfrac{1}{\nu}}$ and$\nu\approx 1.12(6)$ . For all calculations, we take$t_1=1$ ,$\gamma_x= $ $ \gamma_y=0.3$ 
图 2 非厄米局域拓扑指标的传播速度 (a) 淬火过程中系统中心格点处的非厄米局域拓扑指标的时间演化. 系统尺寸为
$L=23$ , 取开边界. 初始时${\boldsymbol{H}}\left(t_1=1,\; m=1\right)$ 处于拓扑非平庸相, 淬火后${\boldsymbol{H}}\left(t^{\prime}_1=1,\; m^{\prime}=6\right)$ 处于拓扑平庸相, 淬火前后$\gamma_x=\gamma_y=0.3$ . 这里只考虑$x$ 方向的动力学演化,$y$ 方向的演化有类似性质. (b) 非厄米局域拓扑指标的传播速度随末态哈密顿量参数$t^{\prime}_1$ 的变化. 淬火参数与图(a)相同. 分别数值模拟了体系大小为$L=11, 15, 19, 23, 27$ 时的淬火过程, 并通过线性拟合$t^\ast$ 与$L$ 的关系, 数值得到了局域拓扑指标的传播速度Figure 2. Dynamics of the non-Hermitian local topological marker. (a) Spatial distribution (along the
$x$ -direction) of the non-Hermitian local topological marker at different times of the quench dynamics. The parameters are:$L=23$ ,${\boldsymbol{H}}_{\rm i}(t_1=1, \;m=1)$ ,${\boldsymbol{H}}_{\rm f}(t'_1=1, \;m'=6)$ ,$\gamma_x=\gamma_y=0.3$ . (b) Propagation speed of the local topological marker as a function of$t'_1$ . Other parameters are the same as those in panel (a).
图 3 模型(5)的非厄米局域拓扑指标的传播速度随
$t^{\prime}_1$ 的变化. 初始时,$t_x=t_y=1, m=1$ ; 淬火后,$t^{\prime}_x=t^{\prime}_y=t^{\prime}_1, $ $ m^{\prime}=6$ . 淬火前后$\gamma_x= \gamma_y=\gamma=0.35$ Figure 3. Propagation speed of the non-Hermitian local topological marker for Hamiltonian (5). We fix
$\gamma_x=\gamma_y=\gamma=0.35$ , and the pre- and post-quench parameters are$t_x=t_y=1, $ $ \; m=1$ and$t^{\prime}_x=t^{\prime}_y=t^{\prime}_1, \; m^{\prime}=6$ , respectively.
图 4 模型(8)的非厄米局域拓扑指标的传播速度随
$t^{\prime}_1$ 的变化. 初始时,$t_x=t_y=1, m=1$ ; 淬火后,$t^{\prime}_x=t^{\prime}_y=t^{\prime}_1, $ $ m^{\prime}=6$ . 淬火前后$\gamma=0.3$ Figure 4. Propagation speed of the non-Hermitian local topological marker for Hamiltonian (8). We fix
$\gamma=0.3$ , and the pre- and post-quench parameters are$t_x=t_y=1, m=1$ and$t^{\prime}_x=t^{\prime}_y=t^{\prime}_1, m^{\prime}=6$ , respectively. -
[1] Ashida Y, Gong Z, Ueda M 2020 Adv. Phys. 69 249
Google Scholar
[2] Kawabata K, Shiozaki k, Ueda M, Sato M 2019 Phys. Rev. X 9 041015
Google Scholar
[3] Zhou H, Lee J Y 2019 Phys. Rev. B 99 235112
Google Scholar
[4] Bender C M 2007 Rep. Prog. Phys. 70 947
Google Scholar
[5] Konotop V V, Yang J, Zezyulin D A 2016 Rev. Mod. Phys. 88 035002
Google Scholar
[6] El-Ganainy R, Makris K G, Khajavikhan M, Musslimani Z H, Rotter S, Christodoulides D N 2017 Nat. Phys. 14 11
Google Scholar
[7] Dalibard J, Castin Y, Mölmer K 1992 Phys. Rev. Lett. 68 580
Google Scholar
[8] Carmichael H J 1993 Phys. Rev. Lett. 70 2273
Google Scholar
[9] Yao S Y, Wang Z 2018 Phy. Rev. Lett. 121 086803
Google Scholar
[10] Yao S Y, Song F, Wang Z 2018 Phys. Rev. Lett. 121 136802
Google Scholar
[11] Lee C H, Thomale R 2019 Phy. Rev. B 99 201103
Google Scholar
[12] McDonald A, Pereg-Barnea T, Clerk A A, 2018 Phys. Rev. X 8 041031
Google Scholar
[13] Kunst F K, Edvardsson E, Budich J C, Bergholtz E J 2018 Phy. Rev. Lett. 121 026808
Google Scholar
[14] Yokomizo K, Murakami S 2019 Phys. Rev. Lett. 123 066404
Google Scholar
[15] Zhang K, Yang Z, Fang C 2020 Phy. Rev. Lett. 125 126402
Google Scholar
[16] Okuma N, Kawabata K, Shiozaki K, Sato M 2020 Phys. Rev. Lett. 124 086801
Google Scholar
[17] Lee T E 2016 Phy. Rev. Lett. 16 133903
Google Scholar
[18] Zhang X Z, Gong J B, 2020 Phy. Rev. B 101 045415
Google Scholar
[19] Zeng Q B, Yang Y B, Xu Y 2020 Phy. Rev. B 101 020201
Google Scholar
[20] Wang X R, Guo C X, Kou S P 2020 Phy. Rev. B 101 121116
Google Scholar
[21] Li T Y, Zhang Y S, Yi W 2021 Chin. Phys. Lett. 38 030301
Google Scholar
[22] Helbig T, Hofmann T, Imhof S, Abdelghany M, Kiessling T, Molenkamp L W, Lee C H, Szameit A, Greiter M, Thomale R 2020 Nat. Phys. 16 747
Google Scholar
[23] Xiao L, Deng T S, Wang K K, Zhu G, Wang Z, Yi W, Xue P 2020 Nat. Phys. 16 761
Google Scholar
[24] Ghatak A, Brandenbourger M, van Wezel J, Coulais C 2020 Proc. Natl. Acad. Sci. U.S.A. 117 29561
Google Scholar
[25] Weidemann S, Kremer M, Helbig T, Hofmann T, Stegmaier A, Greiter M, Thomale R, Szameit A 2020 Science 368 311
Google Scholar
[26] Longhi S 2019 Phys. Rev. Res. 1 023013
Google Scholar
[27] Longhi S 2019 Opt. Lett. 44 5804
Google Scholar
[28] Xiao L, Deng T S, Wang K K, Wang Z, Yi W, Xue P 2021 Phys. Rev. Lett. 126 230402
Google Scholar
[29] Li T Y, Sun J Z, Zhang Y S, Yi W 2021 Phys. Rev. Res. 3 023022
Google Scholar
[30] Wang K, Li T, Xiao L, Han Y, Yi W, Xue P 2021 arXiv: 2107.14741
[31] Luo X W, Zhang C W 2019 arXiv: 1912.10652
[32] Song F, Yao S, Wang Z 2019 Phys. Rev. Lett. 123 246801
Google Scholar
[33] Bianco R, Resta R 2011 Phys. Rev. B 84 241106
Google Scholar
[34] Caio M D, Mller G, Cooper N R, Bhaseen M J 2019 Nat. Phys. 15 257
Google Scholar
[35] Privitera L and Santoro G E 2016 Phy. Rev. B 93 241406
Google Scholar
[36] Pozo O, Repellin C, Grushin A G 2019 Phys. Rev. Lett. 123 247401
Google Scholar
[37] Qi X L, Wu Y S, Zhang S C 2006 Phys. Rev. B 74 085308
Google Scholar
[38] Qi X L, Zhang S C 2011 Rev. Mod. Phys. 83 1057
Google Scholar
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