Broadband periodic and aperiodic acoustic topological insulator based on composite honeycomb structure

Pei Dong-Liang; Yang Tao; Chen Meng; Liu Yu; Xu Wen-Shuai; Zhang Man-Gong; Jiang Heng; Wang Yu-Ren

doi:10.7498/aps.69.20191454

Abstract

The discovery of quantum Hall effect and quantum spin Hall effect has set off a new research upsurge in condensed matter physics. As is analogous to electronic systems, many novel optical and acoustic control devices have been designed by using the defects- immune and backscatter suppression of topological edges in photonic crystals and phononic crystals, which greatly enriches the current physical world and arouses more research enthusiasm. With the study of acoustic topological structure, it has been found that the realization of good reconfigurability, good compatibility against manufacturing defects, and compact acoustic topological insulators may become a promising development direction. This imposes higher requirements on the topological band gap width of the current acoustic topological structure. At the same time, the restriction on the using of the same primitive unit cells in previous researches does not reveal the implementation of aperiodic double Dirac cone topological insulators. Here in this work we present a tunable, two-dimensional broadband composite honeycomb lattice structure for airborne sound. Firstly, We construct a hexagonal structure and then take a circle with a radius of r₁ in the center. Then the circle is anisotropically scaled with the scaling factor s, which means that the x direction of the circle is expanded by $\sqrt s $ times, and the y direction is reduced by $1/\sqrt s $ times to form an ellipse. Then, we perform a translation and rotation transformation on the ellipse, and finally construct a “triangular-like” petal pattern at each vertex of the hexagon. Secondly, we place a circle with a radius of r₂ in the center to achieve the unit cell of the phononic crystal. This cell has two variables. One is the rotation angle θ of the petal pattern around its centroid, and the other is the scaling factor s. We find that there is a quadruple degenerate state at Γ with s = 1.2 and θ = ±33°. On both sides of ±33°, changing θ will induce an inverted band and a topological phase transition. At the same time, the relative band gap of the structure increases gradually. When θ is 0° and 60°, the structures are two topologically distinct broadband phononic crystals with relative band widths of 0.39 and 0.33, respectively. Calculated by the finite element software Comsol, the edge states existing in the band gap are found, and the backscattering immunity characteristics of the topological edges to defects such as right angle, Z-angle, disorder, and cavity are confirmed. For the first time we construct a aperiodic double Dirac cone acoustic topological insulators with different values of s and change their defect immunity. The research system is rich in function, and its relative bandwidth can even exceed 0.5 for a certain s value, which significantly exceeds the bandwidth of the known structure, and lays a good foundation for miniaturized acoustic wave devices taking full advantage of acoustic topological edges. Meanwhile, the realization of aperiodic topological insulators shows that the system can be used more flexibly for acoustic structure design.

Keywords:

topological phase transition /
broadband structure /
aperiodic double Dirac cone topological insulator

Authors and contacts

1.
Key Laboratory of Microgravity, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China
2.
University of Chinese Academy of Sciences, Beijing 100049, China
3.
Wuhan Second Ship Design and Research Institute, Hubei 430064, China

Corresponding author: Chen Meng, chenmeng@imech.ac.cn ; Jiang Heng, hengjiang@imech.ac.cn ;

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 11602269, 11972034, 11802213), the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant No. XDB22040301), and the Research Program of Beijing, China (Grant Nos. Z161100002616034, Z171100000817010)

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References

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Cited By

图 1 (a)正六边形表示晶格的元胞, 其中a₁, a₂是晶格基矢. 在六边形顶点的蓝色“花瓣”形结构与位于中心的圆形结构表示位于空气中的硬质散射体; (b)晶格的最简布里渊区Γ-M-K; (c)晶格结构的示意图

Figure 1. (a) The hexagon represents the cell of the lattice, where a₁, a₂ is the lattice basis vector, the blue “petal” shape at the apex of the hexagon and the circular structure at the center represent the hard scatterers surrounded by air; (b) the irreducible Brillouin zone Γ-M-K; (c) schematic diagram of crystal structure.

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图 2 CHL不同转角时的频带图与其拓扑相变　(a) θ = 0°, 其中下面两幅插图表示d态的声压场分布, 上面两幅插图表示p态的声压场分布; (b) θ = 60°, 插图表示p, d态的声压场分布; (c)结构的拓扑相图, 表示随着转角变化, 频带发生反转; (d)不同转角下带隙的相对带宽

Figure 2. The band structures with different θ and its topological phase transition of the CHL: (a) θ = 0°, in which the lower two illustrations show the sound pressure field distribution of the d state, and the upper two illustrations show the sound pressure field distribution of the p state; (b) θ = 60°, in which the upper and lower illustrations show the sound pressure field distribution of the d and p states, respectively; (c) the topological phase diagram of the structure, indicating that the frequency band is reversed as the rotation angle changes; (d) the relative bandwidth of the band gap at different θ.

DownLoad: Full-Size Img PowerPoint

图 3 (a) Ⅰ型边界沿k_x方向的投影带结构, 图中的灰色区域表示体态, 红色点线表示边界态, 两侧插图表示θ = 60°的5层平庸型声子晶体与θ = 0°的5层非平庸型声子晶体沿着k_y方向拼接起来, 构成的超胞及a₁, a₂, b₁, b₂点的声压分布; (b) Ⅱ型边界沿k_y方向的投影带结构, 两侧插图表示θ = 60°的10层平庸型声子晶体与θ = 0°的10层非平庸型声子晶体沿着k_x方向拼接起来, 构成的超胞及c₁, c₂, d₁, d₂点的声压分布, 插图中的黑色弧形箭头表示边界处的能流方向

Figure 3. (a) The projection band structure of the type I edge along the k_x direction. The gray area in the figure represents the bulk state, and the red dotted line represents the edge state. The illustrations on both sides indicate that the five-layer trivial phononic crystal with θ = 60° and the five-layer nontrivial phononic crystal with θ = 0° are spliced along the k_y direction to form the supercell and the sound pressure distribution at a₁, a_2, b₁, b₂; (b) the projection band structure of the type II edge along the k_y direction. The illustrations on both sides indicate that a 10-layer trivial phononic crystal with θ = 60° and a 10-layer nontrivial phononic crystal with θ = 0° are spliced together in the k_x direction to form the supercell and the sound pressure distribution at points c_1, c₂, d₁, d₂. The black curved arrow in the illustration indicates the energy flow direction at the edge.

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图 4 幅值为1, f = 6900 Hz的平面波从左侧入时结构的声压分布及透射谱　(a)由θ = 60°与θ = 0°的声子晶体的拼接结构组成的混合声子晶体, 两种声子晶体的相接触的边界称为拓扑边界, 左侧的青色箭头表示平面波入射, 从图中声压分布可以看出: 声波能够绕过直角与Z形角沿着边界进行传播; (b)在图(a)的基础上继续引入乱序与缺失的缺陷, 声波依然能够绕过这些缺陷传播; (c)由θ = 60°声子晶体单独构成的结构, 声波不能传播; (d)图(a)—图(c)结构的声强透射谱

Figure 4. The sound pressure distribution and transmission spectrum of the structure when a plane wave is incident from the left side with amplitude 1 Pa and f = 6900 Hz: (a) A mixed phononic crystal composed of a spliced structure of phononic crystals with θ = 60° and θ = 0°, and the edge between the two phononic crystals is called the topological edge. The cyan arrow on the left side indicates the plane wave incidence. It can be seen from the sound pressure distribution that the sound wave can propagate around the right angle and the Z-angle along the edge; (b) introduce disorder and cavity on the basis of Fig. (a), sound waves can still propagate around these defects; (c) a structure consisted of phononic crystals with θ = 60° alone where sound waves cannot propagate; (d) sound intensity transmission spectra of the structures of Fig. (a)—Fig. (c).

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图 5 (a) Γ处d, p态对应的频率值随s的变化情况; (b) s = 0.8时结构的拓扑相图; (c) s = 1.2时结构的拓扑相图

Figure 5. (a) The frequency corresponding to the d and p states with the changes of the parameter s at Γ; (b) the topological phase diagram of the structure at s = 0.8; (c) the topological phase diagram of the structure at s = 1.2.

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图 6 非周期拓扑绝缘体结构的声压分布　(a)为由s为0.8, 1.0, 1.2三种声子晶体构造的非周期声拓扑绝缘体组成及其在右侧f = 6900 Hz声波入射下的声压幅值分布. 中间的横虚线表示水平拼接位置, 竖虚线表示竖直拼接位置, 第一、二幅插图代表θ为0°, s为0.8, 1.0时, 晶格的元胞. 三种声子晶体的具体位置如第三幅插图所示, 其中A, B, C分别表示s为0.8, 1.0, 1.2三种结构, 数字1, 2分别代表θ为0°, 60°两种不同的转角, 右侧的青色箭头代表平面波入射; (b)表示x = 20a处沿着y方向的声压幅值分布, 其值经过最大值归一化; (c)在图(a)的基础上进一步引入乱序与缺失的缺陷时结构声压幅值的分布

Figure 6. Sound pressure distribution of aperiodic topological insulator structure: (a) A periodic acoustic topological insulator composed of three phononic crystal structures with s = 0.8, 1.0, and 1.2 and its sound pressure amplitude distribution when sound wave with f = 6900 Hz is incident from the right side. The horizontal dashed line in the middle indicates the horizontal stitching position, and the vertical dashed line indicates the vertical stitching position. The first and second insets represent the lattice cells with θ = 0° and s of 0.8 and 1.0, respectively. The specific positions of the three phononic crystals are shown in the third illustration, where A, B, and C respectively represent s = 0.8, 1.0, and 1.2, and the numbers 1 and 2 represent θ = 0° and 60°, respectively. The cyan arrow on the right indicates the incident plane wave; (b) the sound pressure amplitude distribution along the y direction at x = 20a, and its value is normalized by the maximum value; (c) the distribution of the sound pressure amplitude when introducing disorder and cavity on the basis of Fig. (a).

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map

[1]	Gusynin V P, Sharapov S G 2005 Phys. Rev. Lett. 95 146801 Google Scholar
[2]	Zhang Y, Tan Y W, Stormer H L, Kim P 2005 Nature 438 201 Google Scholar
[3]	Peres N M R, Guinea F, Neto A C 2006 Phys. Rev. B 73 125411 Google Scholar
[4]	Privman V, Vagner I D, Kventsel G 1998 Phys. Lett. A 239 141 Google Scholar
[5]	Klitzing K V, Dorda G, Pepper M 1980 Phys. Rev. Lett. 45 494 Google Scholar
[6]	Laughlin R B 1983 Phys. Rev. Lett. 50 1395 Google Scholar
[7]	Kane C L, Mele E J 2004 Phys. Rev. Lett. 95 226801
[8]	Bernevig B A, Zhang S C 2006 Phys. Rev. Lett. 96 106802 Google Scholar
[9]	Kosterlitz J M, Thouless D J 1972 Solid State Phys. 5 L124 Google Scholar
[10]	Kosterlitz J M, Thouless D J 1973 Solid State Phys. 6 1181 Google Scholar
[11]	Yu R, Zhang W, Zhang H J, Zhang S C, Dai X, Fang Z 2010 Science 329 61 Google Scholar
[12]	Hasan M Z, Kane C L 2010 Rev. Mod. Phys. 82 3045 Google Scholar
[13]	Shen S Q, Shan W Y, Lu H Z 2011 Spin 1 33 Google Scholar
[14]	田源, 葛浩, 卢明辉, 陈延峰 2019 68 194301 Google Scholar Tian Y, Ge H, Lu M H, Chen Y F 2019 Acta Phys. Sin. 68 194301 Google Scholar
[15]	Wang Z, Chong Y D, Joannopoulos J D, Soljacic M 2008 Phys. Rev. Lett. 100 013905 Google Scholar
[16]	Raghu S, Haldane F D M 2008 Phys. Rev. A 78 033834 Google Scholar
[17]	Ochiai T, Onoda M 2009 Phys. Rev. B 80 155103 Google Scholar
[18]	Gao F, Gao Z, Shi X, Yang Z, Lin X, Xu H, Chong Y, Soljačić M, Chen H, Lu L, Zhang B 2016 Nat. Commun. 7 11619 Google Scholar
[19]	Peano V, Brendel C, Schmidt M, Marquardt F 2015 Phys. Rev. X 5 031011
[20]	Gao W, Lawrence M, Yang B, Liu F, Fang F, Béri B, Li J, Zhang S 2015 Phys. Rev. Lett. 114 037402 Google Scholar
[21]	Ma T, Khanikaev A B, Mousavi S H, Shvets G 2015 Phys. Rev. Lett. 114 127401 Google Scholar
[22]	Hafezi M, Mittal S, Fan J, Migdall A, Taylor J M 2013 Nat. Photonics 7 1001 Google Scholar
[23]	Khanikaev A B, Mousavi S H, Tse W K, Kargarian M, MacDonald A H, Shvets G 2013 Nat. Mater. 12 233 Google Scholar
[24]	Wu L H, Hu X 2015 Phys. Rev. Lett. 114 223901 Google Scholar
[25]	Ni X, He C, Sun X C, Liu X. P, Lu M H, Feng L, Chen Y F 2015 New J. Phys. 17 053016
[26]	Yang Z, Gao F, Shi X, Lin X, Gao Z, Chong Y, Zhang B 2015 Phys. Rev. Lett. 114 114301 Google Scholar
[27]	Chen Z G, Wu Y 2016 Phys. Rev. Appl. 5 054021 Google Scholar
[28]	Peng Y G, Qin C Z, Zhao D G, Shen Y X, Xu X Y, Bao M, Jia H, Zhu X F 2016 Nat. Commun. 7 13368 Google Scholar
[29]	Peng Y G, Shen Y X, Zhao D G, Zhu X F 2017 Appl. Phys. Lett. 110 173505 Google Scholar
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[32]	Lu J, Qiu C, Deng W, Huang X, Li F, Zhang F, Liu Z 2018 Phys. Rev. Lett. 120 116802 Google Scholar
[33]	Dai H, Jiao J, Xia B, Liu T, Zheng S, Yu D 2018 J. Phys. D: Appl. Phys. 51 175302 Google Scholar
[34]	Xia B Z, Liu T T, Huang G L, Dai H Q, Jiao J R, Zang X G, Yu D J, Zheng S J, Liu J 2017 Phys. Rev. B 96 094106 Google Scholar
[35]	Geng Z G, Peng Y G, Shen Y X, Zhao D G, Zhu X F 2018 Appl. Phys. Lett. 113 033503 Google Scholar
[36]	Geng Z G, Peng Y G, Li P Q, Shen Y X, Zhao D G, Zhu X F 2019 J. Phys.Condens. Matter 31 245403 Google Scholar
[37]	Zhang Z, Wei Q, Cheng Y, Zhang T, Wu D, Liu X 2017 Phys. Rev. Lett. 118 084303 Google Scholar
[38]	Deng Y, Ge H, Tian Y, Lu M, Jing Y 2017 Phys. Rev. B 96 184305 Google Scholar
[39]	Zhang Z, Tian Y, Cheng Y, Liu X, Christensen J 2017 Phys. Rev. B 96 241306 Google Scholar
[40]	Zhang Z, Tian Y, Cheng Y, Wei Q, Liu X, Christensen J 2018 Phys. Rev. Appl. 9 034032 Google Scholar
[41]	Xia J P, Jia D, Sun H X, Yuan S Q, Ge Y, Si Q R, Liu X J 2018 Adv. Mater. 30 1805002 Google Scholar
[42]	Mei J, Chen Z, Wu Y 2016 Sci. Rep. 6 32752 Google Scholar
[43]	Dai H, Qian M, Jiao J, Xia B, Yu D 2018 J. Appl. Phys. 124 175107 Google Scholar
[44]	Han X, Peng Y G, Li L, Hu Y, Mei C, Zhao D G, Zhu X F, Wang X 2019 Phys. Rev. Appl. 12 014046 Google Scholar

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