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Generation of higher-order topological insulators using periodic driving

Ghosh, Arnob Kumar (författare)
Uppsala universitet,Materialteori,Inst Phys, Sachivalaya Marg, Bhubaneswar 751005, India; Homi Bhabha Natl Inst, Training Sch Complex, Mumbai 400094, India
Nag, Tanay (författare)
Uppsala universitet,Materialteori,BITS Pilani, Dept Phys, Hyderabad Campus, Hyderabad 500078, Telangana, India
Saha, Arijit (författare)
Inst Phys, Sachivalaya Marg, Bhubaneswar 751005, India; Homi Bhabha Natl Inst, Training Sch Complex, Mumbai 400094, India
 (creator_code:org_t)
Institute of Physics Publishing (IOPP), 2024
2024
Engelska.
Ingår i: Journal of Physics. - : Institute of Physics Publishing (IOPP). - 0953-8984 .- 1361-648X. ; 36:9
  • Forskningsöversikt (refereegranskat)
Abstract Ämnesord
Stäng  
  • Topological insulators (TIs) are a new class of materials that resemble ordinary band insulators in terms of a bulk band gap but exhibit protected metallic states on their boundaries. In this modern direction, higher-order TIs (HOTIs) are a new class of TIs in dimensions d > 1. These HOTIs possess -dimensional boundaries that, unlike those of conventional TIs, do not conduct via gapless states but are themselves TIs. Precisely, an nth order d-dimensional higher-order TI is characterized by the presence of boundary modes that reside on its -dimensional boundary. For instance, a three-dimensional second (third) order TI hosts gapless (localized) modes on the hinges (corners), characterized by . Similarly, a second-order TI (SOTI) in two dimensions only has localized corner states (). These higher-order phases are protected by various crystalline as well as discrete symmetries. The non-equilibrium tunability of the topological phase has been a major academic challenge where periodic Floquet drive provides us golden opportunity to overcome that barrier. Here, we discuss different periodic driving protocols to generate Floquet HOTIs while starting from a non-topological or first-order topological phase. Furthermore, we emphasize that one can generate the dynamical anomalous π-modes along with the concomitant 0-modes. The former can be realized only in a dynamical setup. We exemplify the Floquet higher-order topological modes in two and three dimensions in a systematic way. Especially, in two dimensions, we demonstrate a Floquet SOTI (FSOTI) hosting 0- and π corner modes. Whereas a three-dimensional FSOTI and Floquet third-order TI manifest one- and zero-dimensional hinge and corner modes, respectively.

Ämnesord

NATURVETENSKAP  -- Fysik -- Den kondenserade materiens fysik (hsv//swe)
NATURAL SCIENCES  -- Physical Sciences -- Condensed Matter Physics (hsv//eng)

Nyckelord

ID
generation
higher-order
topological
insulators
periodic
Floquet systems

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Ghosh, Arnob Kum ...
Nag, Tanay
Saha, Arijit
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NATURVETENSKAP
NATURVETENSKAP
och Fysik
och Den kondenserade ...
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Journal of Physi ...
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Uppsala universitet

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