Author
Listed:
- Kazuhiro Nawa
(Tohoku University)
- Kimihiko Tanaka
(Tokyo Institute of Technology)
- Nobuyuki Kurita
(Tokyo Institute of Technology)
- Taku J. Sato
(Tohoku University)
- Haruki Sugiyama
(Tokyo Institute of Technology)
- Hidehiro Uekusa
(Tokyo Institute of Technology)
- Seiko Ohira-Kawamura
(J-PARC Center)
- Kenji Nakajima
(J-PARC Center)
- Hidekazu Tanaka
(Tokyo Institute of Technology)
Abstract
Search for topological materials has been actively promoted in the field of condensed matter physics for their potential application in energy-efficient information transmission and processing. Recent studies have revealed that topologically invariant states, such as edge states in topological insulators, can emerge not only in a fermionic electron system but also in a bosonic system, enabling nondissipative propagation of quasiparticles. Here we report the topologically nontrivial triplon bands measured by inelastic neutron scattering on the spin-1/2 two-dimensional dimerized antiferromagnet Ba2CuSi2O6Cl2. The excitation spectrum exhibits two triplon bands that are clearly separated by a band gap due to a small alternation in interdimer exchange interaction, consistent with a refined crystal structure. By analytically modeling the triplon dispersion, we show that Ba2CuSi2O6Cl2 is the first bosonic realization of the coupled Su-Schrieffer-Heeger model, where the presence of topologically protected edge states is prompted by a bipartite nature of the lattice.
Suggested Citation
Kazuhiro Nawa & Kimihiko Tanaka & Nobuyuki Kurita & Taku J. Sato & Haruki Sugiyama & Hidehiro Uekusa & Seiko Ohira-Kawamura & Kenji Nakajima & Hidekazu Tanaka, 2019.
"Triplon band splitting and topologically protected edge states in the dimerized antiferromagnet,"
Nature Communications, Nature, vol. 10(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:10:y:2019:i:1:d:10.1038_s41467-019-10091-6
DOI: 10.1038/s41467-019-10091-6
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