2019
DOI: 10.1016/j.jmps.2019.01.009
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Inverse design of quantum spin hall-based phononic topological insulators

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Cited by 87 publications
(33 citation statements)
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“…These experimental results differ from all of the prior research [15,[27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] that have only demonstrated the twoway partitioning of topological modes. Our design is wholly contingent upon the geometrical properties of the square and rectangular lattices.…”
Section: B Three-way Beam Splitting For Topological Acoustic Modescontrasting
confidence: 99%
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“…These experimental results differ from all of the prior research [15,[27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] that have only demonstrated the twoway partitioning of topological modes. Our design is wholly contingent upon the geometrical properties of the square and rectangular lattices.…”
Section: B Three-way Beam Splitting For Topological Acoustic Modescontrasting
confidence: 99%
“…Numerous examples of two-way beam splitters have been shown [15,[27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] that leverage the geometry of graphenelike hexagonal structures. The restriction to two-way beam splitting is due to a conservation of a topological charge inherent within graphenelike structures [17]; to obtain these three-way beam splitters, square, or rectangular, lattice structures must be used and not the hexagonal graphenelike structures that are prevalent in the topological community [15,[27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42]. Venturing beyond beam splitters, a longstanding desire within the phononic's sister photonics community has been to mold the flow of light through and around complex optoelectronic "photonic cities," as shown on the cover of the now classic book by Joannopoulos et al [43].…”
Section: Introductionmentioning
confidence: 99%
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“…Considerable progress was made in the experimental realization of such states in all the above mentioned areas, in particular in electronic systems (see refs. [] and references therein), where such states were introduced initially, mechanical systems, where tunable phononic topological insulators have been designed using geometrically induced effects of spin–orbit coupling,, acoustics, cold atoms in optical lattices, atomic Bose–Einstein condensates, and most notably in optical systems (see ref. []), including gyromagnetic photonic crystals, semiconductor quantum wells, arrays of coupled resonators, metamaterial superlattices, and helical waveguide arrays .…”
Section: Introductionmentioning
confidence: 99%
“…Inverse design methods adopt topology and shape optimization to meet requirements like larger topological band width and flexible operating frequency ranges. The inverse design approaches are based on achieving intended unit cell band structure [22,23] or localizing energy in specific paths of the periodic structure [24]. Reconfigurability or tunability by the presence of buckling members in lattices [25], pre-stressing soft phononic crystals [26] or embedding shunted piezoelectric patches [27,28] overcomes the constraint of fixed wave paths in case of passive phononic metamaterials.…”
Section: Introductionmentioning
confidence: 99%