scholarly journals Edge-state influence on high-order harmonic generation in topological nanoribbons

2021 ◽  
Vol 75 (6) ◽  
Author(s):  
Christoph Jürß ◽  
Dieter Bauer

Abstract The high-order harmonic generation in finite topological nanoribbons is investigated using a tight-binding approximation. The narrow, two-dimensional ribbons consist of hexagonal structures. A topological phase transition is defined by a sudden change of the topological invariant. In the bulk, this kind of phase transition might occur if an existing band gap closes and reopens again. Through the bulk-boundary correspondence, this is related to the emergence of topologically protected edge states in the respective finite systems. For the finite ribbons studied in this work, the variation of the tight-binding parameters leads to the emergence of two edge states after the closing of the band gap. The energies of those edge states as functions of the tight-binding parameters display crossings and avoided crossings, which influence the high-harmonic spectra. Graphic Abstract

2020 ◽  
Vol 45 (10) ◽  
pp. 2874 ◽  
Author(s):  
Yi-Ting Zhao ◽  
Shi-Cheng Jiang ◽  
Xi Zhao ◽  
Ji-Gen Chen ◽  
Yu-Jun Yang

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Jeng-Rung Jiang ◽  
Wei-Ting Chen ◽  
Ruey-Lin Chern

Abstract We investigate the parity-time (PT) phase transition in photonic crystals with $$C_{6v}$$ C 6 v symmetry, with balanced gain and loss on dielectric rods in the triangular lattice. A two-level non-Hermitian model that incorporates the gain and loss in the tight-binding approximation was employed to describe the dispersion of the PT symmetric system. In the unbroken PT phase, the double Dirac cone feature associated with the $$C_{6v}$$ C 6 v symmetry is preserved, with a frequency shift of second order due to the presence of gain and loss. The helical edge states with real eigenfrequencies can exist in the common band gap for two topologically distinct lattices. In the broken PT phase, the non-Hermitian perturbation deforms the dispersion by merging the frequency bands into complex conjugate pairs and forming the exceptional contours that feature the PT phase transition. In this situation, the band gap closes and the edge states are mixed with the bulk states.


2003 ◽  
Vol 50 (3-4) ◽  
pp. 375-386
Author(s):  
D. B. MilosÕeviĆ ◽  
W. Becker

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