Dirac point in the photon dispersion relation of a negative/zero/positive-index plasmonic metamaterial

2011 ◽  
Vol 84 (4) ◽  
Author(s):  
Vassilios Yannopapas ◽  
Alexandros Vanakaras
2010 ◽  
Vol 18 (12) ◽  
pp. 12779 ◽  
Author(s):  
Ming Shen ◽  
Lin-Xu Ruan ◽  
Xi Chen

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
A. Valdés-Curiel ◽  
D. Trypogeorgos ◽  
Q.-Y. Liang ◽  
R. P. Anderson ◽  
I. B. Spielman

AbstractTopological order can be found in a wide range of physical systems, from crystalline solids, photonic meta-materials and even atmospheric waves to optomechanic, acoustic and atomic systems. Topological systems are a robust foundation for creating quantized channels for transporting electrical current, light, and atmospheric disturbances. These topological effects are quantified in terms of integer-valued ‘invariants’, such as the Chern number, applicable to the quantum Hall effect, or the $${{\mathbb{Z}}}_{2}$$ Z 2 invariant suitable for topological insulators. Here, we report the engineering of Rashba spin-orbit coupling for a cold atomic gas giving non-trivial topology, without the underlying crystalline structure that conventionally yields integer Chern numbers. We validated our procedure by spectroscopically measuring both branches of the Rashba dispersion relation which touch at a single Dirac point. We then measured the quantum geometry underlying the dispersion relation using matter-wave interferometry to implement a form of quantum state tomography, giving a Berry’s phase with magnitude π. This implies that opening a gap at the Dirac point would give two dispersions (bands) each with half-integer Chern number, potentially implying new forms of topological transport.


Author(s):  
Xiujuan Zhang ◽  
Ying Wu

A semi-Dirac cone refers to a peculiar type of dispersion relation that is linear along the symmetry line but quadratic in the perpendicular direction. It was originally discovered in electron systems, in which the associated quasi-particles are massless along one direction, like those in graphene, but effective-mass-like along the other. It was reported that a semi-Dirac point is associated with the topological phase transition between a semi-metallic phase and a band insulator. Very recently, the classical analogy of a semi-Dirac cone has been reported in an electromagnetic system. Here, we demonstrate that, by accidental degeneracy, two-dimensional phononic crystals consisting of square arrays of elliptical cylinders embedded in water are also able to produce the particular dispersion relation of a semi-Dirac cone in the center of the Brillouin zone. A perturbation method is used to evaluate the linear slope and to affirm that the dispersion relation is a semi-Dirac type. If the scatterers are made of rubber, in which the acoustic wave velocity is lower than that in water, the semi-Dirac dispersion can be characterized by an effective medium theory. The effective medium parameters link the semi-Dirac point to a topological transition in the iso-frequency surface of the phononic crystal, in which an open hyperbola is changed into a closed ellipse. This topological transition results in drastic change in wave manipulation. On the other hand, the theory also reveals that the phononic crystal is a double-zero-index material along the x-direction and photonic-band-edge material along the perpendicular direction (y-direction). If the scatterers are made of steel, in which the acoustic wave velocity is higher than that in water, the effective medium description fails, even though the semi-Dirac dispersion relation looks similar to that in the previous case. Therefore different wave transport behavior is expected. The semi-Dirac points in phononic crystals described in this work would offer new ways to manipulate acoustic waves with simple periodic structures.


2011 ◽  
Vol 83 (4) ◽  
Author(s):  
Ming Shen ◽  
Linxu Ruan ◽  
Xinglin Wang ◽  
Jielong Shi ◽  
Qi Wang

2010 ◽  
Vol 12 (8) ◽  
pp. 085201 ◽  
Author(s):  
Ming Shen ◽  
Lin-Xu Ruan ◽  
Xi Chen ◽  
Jie-Long Shi ◽  
Hai-Xia Ding ◽  
...  

2021 ◽  
pp. 150182
Author(s):  
Maosheng Yang ◽  
Tengteng Li ◽  
Ju Gao ◽  
Xin Yan ◽  
Lanju Liang ◽  
...  

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