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Professor Xu Gang invited Liu Feng Academy of Kansai University in Japan to make a report

Release Time: 2019-04-15 17:15


Title: Topological dipoles and quadrupoles

Speaker: Liu Feng Special Researcher

        Kansai University of Japan

Time: 10:00 am, Friday, January 4, 2019

Location: National Pulse Strong Magnetic Field Science Center B206



Abstract :

Topology offers us a unique dimension of designing solid-state materials. One famous example is the Quantum spin Hall effect (QSHE) where electrons of opposite spins propagate oppositely. The origin of QSHE comes from a geometric field strength in momentum space that is the so-called Berry curvature. Besides QSHE, the geometric vector potential whose curl yields the Berry curvature – the Berry connection, can induce an electric dipole even without Berry curvature. The topological electric dipoles result fractional surface charges that manifest as topological edge states, which are robust to defects and edge roughness. Furthermore, a pair of such the topological dipoles can form a high order multipole – quadrupole, which corresponds to the topological corner states. In this talk we will discuss a simple tight-binding model that possesses topological dipoles and quadrupoles in zero Berry curvature [1]. Experimental realizations based on solid-state material and dielectric photonic crystal are proposed [2]. Furthermore, we show that in a pure quadrupole phase, topological edge state is pseudo-spin polarized in general [3].

references:

1.F. Liu and K. Wakabayashi, Phys. Rev. Lett. 118, 076803 (2017).

2.F. Liu, H.-Y. Deng and K. Wakabayashi, Phys. Rev. B 97, 035442 (2018).

3.F. Liu, H.-Y. Deng and K. Wakabayashi, arxiv: 1809.10824


Speaker introduction:

Feng Liu finished his Ph.D. research at National Institute of Materials Sciences (Japan) and received his Ph.D. from University of Tsukuba in 2015. Now he is doing postdoctoral research as a JSPS Fellowship at Kwansei Gakuin University, Japan. His research interests include superconductivity and topological states in condensed-matter and photonic systems.