Photonic topological insulator

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Photonic topological insulators are artificial electromagnetic materials that support topologically non-trivial, unidirectional states of light. [1] Photonic topological phases are classical electromagnetic wave analogues of electronic topological phases studied in condensed matter physics. Similar to their electronic counterparts, they, can provide robust unidirectional channels for light propagation. [2] The field that studies these phases of light is referred to as topological photonics.

Contents

History

Topological order in solid state systems has been studied in condensed matter physics since the discovery of integer quantum Hall effect. But topological matter attracted considerable interest from the physics community after the proposals for possible observation of symmetry-protected topological phases (or the so-called topological insulators ) in graphene, [3] and experimental observation of a 2D topological insulator in CdTe/HgTe/CdTe quantum wells in 2007. [4] [5]

In 2008, Haldane and Raghu proposed that unidirectional electromagnetic states analogous to (integer) quantum Hall states can be realized in nonreciprocal magnetic photonic crystals. [6] This prediction was first realized in 2009 in the microwave frequency regime. [7] This was followed by the proposals for analogous quantum spin Hall states of electromagnetic waves that are now known as photonic topological insulators. [8] [9] It was later found that topological electromagnetic states can exist in continuous media as well--theoretical and numerical study has confirmed the existence of topological Langmuir-cyclotron waves in continuous magnetized plasmas. [10] [11]

Platforms

Photonic topological insulators are designed using various photonic platforms including optical waveguide arrays, [12] coupled ring resonators, [13] bi-anisotropic meta-materials, and photonic crystals. [14] More recently, they have been realized in 2D dielectric [15] and plasmonic [16] meta-surfaces. Despite the theoretical prediction, [10] [11] no experimental demonstration of photonic topological insulator in continuous media has been reported.

Chern number

As an important figure of merit for characterizing the quantized collective behaviors of the wavefunction, Chern number is the topological invariant of quantum Hall insulators. Chern number also identifies the topological properties of the photonic topological insulators (PTIs), thus it is of crucial importance in PTI design. The full-wave finite-difference frequency-domain (FDFD) method based MATLAB program for computing the Chern number has been written. [17] Recently, the finite-difference method has been extended to analyze the topological invariant of non-Hermitian topological dielectric photonic crystals by first-principle Wilson loop calculation. [18] All MATLAB codes can be found at GitHub website. [19]

See also

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References

  1. ↑ Lu, Ling; Joannopoulos, John D.; Soljačić, Marin (November 2014). "Topological photonics". Nature Photonics. 8 (11): 821–829. arXiv: 1408.6730 . Bibcode:2014NaPho...8..821L. doi:10.1038/nphoton.2014.248. ISSN   1749-4893. S2CID   119191655.
  2. ↑ Ozawa, Tomoki; Price, Hannah M.; Amo, Alberto; Goldman, Nathan; Hafezi, Mohammad; Lu, Ling; Rechtsman, Mikael C.; Schuster, David; Simon, Jonathan; Zilberberg, Oded; Carusotto, Iacopo (25 March 2019). "Topological photonics". Reviews of Modern Physics. 91 (1): 015006. arXiv: 1802.04173 . Bibcode:2019RvMP...91a5006O. doi:10.1103/RevModPhys.91.015006. S2CID   10969735.
  3. ↑ Kane, C. L.; Mele, E. J. (23 November 2005). "Quantum Spin Hall Effect in Graphene". Physical Review Letters. 95 (22): 226801. arXiv: cond-mat/0411737 . Bibcode:2005PhRvL..95v6801K. doi:10.1103/PhysRevLett.95.226801. PMID   16384250. S2CID   6080059.
  4. ↑ Bernevig, B. Andrei; Hughes, Taylor L.; Zhang, Shou-Cheng (15 December 2006). "Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells". Science. 314 (5806): 1757–1761. arXiv: cond-mat/0611399 . Bibcode:2006Sci...314.1757B. doi:10.1126/science.1133734. ISSN   0036-8075. PMID   17170299. S2CID   7295726.
  5. ↑ Hasan, M. Z.; Kane, C. L. (8 November 2010). "Colloquium: Topological insulators". Reviews of Modern Physics. 82 (4): 3045–3067. arXiv: 1002.3895 . Bibcode:2010RvMP...82.3045H. doi:10.1103/RevModPhys.82.3045. S2CID   16066223.
  6. ↑ Haldane, F. D. M.; Raghu, S. (10 January 2008). "Possible Realization of Directional Optical Waveguides in Photonic Crystals with Broken Time-Reversal Symmetry". Physical Review Letters. 100 (1): 013904. arXiv: cond-mat/0503588 . Bibcode:2008PhRvL.100a3904H. doi:10.1103/PhysRevLett.100.013904. PMID   18232766. S2CID   44745453.
  7. ↑ Wang, Zheng; et al. (2009). "Observation of unidirectional backscattering-immune topological electromagnetic states". Nature. 461 (7265): 772–775. Bibcode:2009Natur.461..772W. doi:10.1038/nature08293. hdl: 1721.1/88469 . PMID   19812669. S2CID   4427789.
  8. ↑ Hafezi, Mohammad; Demler, Eugene A.; Lukin, Mikhail D.; Taylor, Jacob M. (November 2011). "Robust optical delay lines with topological protection". Nature Physics. 7 (11): 907–912. arXiv: 1102.3256 . Bibcode:2011NatPh...7..907H. doi:10.1038/nphys2063. ISSN   1745-2481. S2CID   2008767.
  9. ↑ Khanikaev, Alexander B.; Hossein Mousavi, S.; Tse, Wang-Kong; Kargarian, Mehdi; MacDonald, Allan H.; Shvets, Gennady (March 2013). "Photonic topological insulators". Nature Materials. 12 (3): 233–239. arXiv: 1204.5700 . Bibcode:2013NatMa..12..233K. doi:10.1038/nmat3520. ISSN   1476-4660. PMID   23241532.
  10. 1 2 Qin, Hong; Fu, Yichen (2023-03-31). "Topological Langmuir-cyclotron wave". Science Advances. 9 (13): eadd8041. doi:10.1126/sciadv.add8041. ISSN   2375-2548. PMC   10065437 . PMID   37000869.
  11. 1 2 Fu, Yichen; Qin, Hong (2021-06-24). "Topological phases and bulk-edge correspondence of magnetized cold plasmas". Nature Communications. 12 (1): 3924. doi:10.1038/s41467-021-24189-3. ISSN   2041-1723. PMC   8225675 . PMID   34168159.
  12. ↑ Rechtsman, Mikael; et al. (April 10, 2013). "Photonic Floquet Topological Insulators". Nature. 496 (7444): 196–200. arXiv: 1212.3146 . Bibcode:2013Natur.496..196R. doi:10.1038/nature12066. PMID   23579677. S2CID   4349770.
  13. ↑ Hafezi, M.; Mittal, S.; Fan, J.; Migdall, A.; Taylor, J. M. (December 2013). "Imaging topological edge states in silicon photonics". Nature Photonics. 7 (12): 1001–1005. arXiv: 1302.2153 . Bibcode:2013NaPho...7.1001H. doi:10.1038/nphoton.2013.274. ISSN   1749-4893. S2CID   14394865.
  14. ↑ Wu, Long-Hua; Hu, Xiao (3 June 2015). "Scheme for Achieving a Topological Photonic Crystal by Using Dielectric Material". Physical Review Letters. 114 (22): 223901. arXiv: 1503.00416 . Bibcode:2015PhRvL.114v3901W. doi:10.1103/PhysRevLett.114.223901. PMID   26196622.
  15. ↑ Gorlach, Maxim A.; Ni, Xiang; Smirnova, Daria A.; Korobkin, Dmitry; Zhirihin, Dmitry; Slobozhanyuk, Alexey P.; Belov, Pavel A.; Alù, Andrea; Khanikaev, Alexander B. (2 March 2018). "Far-field probing of leaky topological states in all-dielectric metasurfaces". Nature Communications. 9 (1): 909. Bibcode:2018NatCo...9..909G. doi: 10.1038/s41467-018-03330-9 . ISSN   2041-1723. PMC   5834506 . PMID   29500466.
  16. ↑ Honari-Latifpour, Mostafa; Yousefi, Leila (2019). "Topological plasmonic edge states in a planar array of metallic nanoparticles". Nanophotonics. 8 (5): 799–806. Bibcode:2019Nanop...8..230H. doi: 10.1515/nanoph-2018-0230 . ISSN   2192-8614.
  17. ↑ Zhao, Ran; Xie, Guo-Da; Chen, Menglin L. N.; Lan, Zhihao; Huang, Zhixiang; Sha, Wei E. I. (2020-02-17). "First-principle calculation of Chern number in gyrotropic photonic crystals". Optics Express. 28 (4): 4638–4649. arXiv: 2001.08913 . Bibcode:2020OExpr..28.4638Z. doi:10.1364/OE.380077. ISSN   1094-4087. PMID   32121697. S2CID   210911652.
  18. ↑ Chen, Menglin L. N.; Jiang, Li Jun; Zhang, Shuang; Zhao, Ran; Lan, Zhihao; Sha, Wei E. I. (2021-09-01). "Comparative study of Hermitian and non-Hermitian topological dielectric photonic crystals". Physical Review A. 104 (3): 033501. arXiv: 2109.05498 . Bibcode:2021PhRvA.104c3501C. doi:10.1103/PhysRevA.104.033501. S2CID   237492242.
  19. ↑ Topological-Invariant-Optics
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