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Ablowitz MJ, Nixon SD, Cole JT. Switching via wave interaction in topological photonic lattices. OPTICS LETTERS 2024; 49:734-737. [PMID: 38300102 DOI: 10.1364/ol.510326] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/21/2023] [Accepted: 01/02/2024] [Indexed: 02/02/2024]
Abstract
A honeycomb Floquet lattice with helically rotating waveguides and an interface separating two counter-propagating subdomains is analyzed. Two topologically protected localized waves propagate unidirectionally along the interface. Switching can occur when these interface modes reach the edge of the lattice and the light splits into waves traveling in two opposite directions. The incoming mode, traveling along the interface, can be adjusted and routed entirely or partially along either lattice edge with the switching direction based on a suitable mixing of the interface modes.
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Bazhan N, Malomed B, Yakimenko A. Josephson oscillations of edge quasi-solitons in a photonic-topological coupler. OPTICS LETTERS 2021; 46:6067-6070. [PMID: 34913919 DOI: 10.1364/ol.445298] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/11/2021] [Accepted: 11/16/2021] [Indexed: 06/14/2023]
Abstract
We introduce a scheme of a photonic coupler built of two parallel topological-insulator slab waveguides with the intrinsic Kerr nonlinearity, separated by a lattice spacing. Josephson oscillations (JOs) of a single edge quasi-soliton (QS) created in one slab, and of a pair of QSs created in two slabs, are considered. The single QS jumping between the slabs is subject to quick radiative decay. However, the JOs of the co-propagating QS pair may be essentially more robust, as one QS absorbs dispersive waves emitted by the other. The most robust JO regime is featured by the pair of QSs with phase shift π between them.
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Sun CL, Li J, Song QW, Ma Y, Zhang ZQ, De JB, Liao Q, Fu H, Yao J, Zhang HL. Lasing from an Organic Micro-Helix. Angew Chem Int Ed Engl 2020; 59:11080-11086. [PMID: 32219946 DOI: 10.1002/anie.202002797] [Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/23/2020] [Indexed: 11/10/2022]
Abstract
Organic solid-state semiconductor lasers are attracting ever-increasing interest for their potential application in future photonic circuits. Despite the great progress made in recent years, an organic laser from 3D chiral structures has not been achieved. Now, the first example of an organic nano-laser from the micro-helix structure of an achiral molecule is presented. Highly regular micro-helixes with left/right-handed helicity from a distyrylbenzene derivative (HM-DSB) were fabricated and characterized under microscope spectrometers. These chiral micro-helixes exhibit unique photonic properties, including helicity-dependent circularly polarized luminescence (CPL), periodic optical waveguiding, and length-dependent amplified spontaneous emission (ASE) behavior. The successful observation of laser behavior from the organic micro-helix extends our understanding to morphology chirality of organic photonic materials and provides a new design strategy towards chiral photonic circuits.
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Affiliation(s)
- Chun-Lin Sun
- State Key Laboratory of Applied Organic Chemistry (SKLAOC), Key Laboratory of Special Function Materials and Structure Design (MOE), College of Chemistry and Chemical Engineering, Lanzhou University, Lanzhou, 730000, P. R. China
| | - Jun Li
- MOE Key Laboratory of Material Physics and Chemistry under Extraordinary Conditions, School of Chemistry and Chemical Engineering, Northwestern Polytechnical University, Xi'an, 710072, P. R. China
| | - Qi-Wei Song
- State Key Laboratory of Applied Organic Chemistry (SKLAOC), Key Laboratory of Special Function Materials and Structure Design (MOE), College of Chemistry and Chemical Engineering, Lanzhou University, Lanzhou, 730000, P. R. China
| | - Yu Ma
- MOE Key Laboratory of Material Physics and Chemistry under Extraordinary Conditions, School of Chemistry and Chemical Engineering, Northwestern Polytechnical University, Xi'an, 710072, P. R. China
| | - Ze-Qi Zhang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC), Key Laboratory of Special Function Materials and Structure Design (MOE), College of Chemistry and Chemical Engineering, Lanzhou University, Lanzhou, 730000, P. R. China
| | - Jian-Bo De
- Beijing Key Laboratory for Optical Materials and Photonic Devices, Department of Chemistry, Capital Normal University, Beijing, 100048, P. R. China
| | - Qing Liao
- Beijing Key Laboratory for Optical Materials and Photonic Devices, Department of Chemistry, Capital Normal University, Beijing, 100048, P. R. China
| | - Hongbing Fu
- Beijing Key Laboratory for Optical Materials and Photonic Devices, Department of Chemistry, Capital Normal University, Beijing, 100048, P. R. China.,Tianjin Key Laboratory of Molecular Optoelectronic Sciences, Department of Chemistry, Tianjin University, and Collaborative, Innovation Center of Chemical Science and Engineering (Tianjin), Tianjin, 300072, P. R. China
| | - Jiannian Yao
- Beijing National Laboratory for Molecules Science (BNLMS), State Key Laboratory for Structural Chemistry of Unstable and Stable Species, Key Laboratory of Photochemistry, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China.,Tianjin Key Laboratory of Molecular Optoelectronic Sciences, Department of Chemistry, Tianjin University, and Collaborative, Innovation Center of Chemical Science and Engineering (Tianjin), Tianjin, 300072, P. R. China
| | - Hao-Li Zhang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC), Key Laboratory of Special Function Materials and Structure Design (MOE), College of Chemistry and Chemical Engineering, Lanzhou University, Lanzhou, 730000, P. R. China.,Tianjin Key Laboratory of Molecular Optoelectronic Sciences, Department of Chemistry, Tianjin University, and Collaborative, Innovation Center of Chemical Science and Engineering (Tianjin), Tianjin, 300072, P. R. China
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Sun C, Li J, Song Q, Ma Y, Zhang Z, De J, Liao Q, Fu H, Yao J, Zhang H. Lasing from an Organic Micro‐Helix. Angew Chem Int Ed Engl 2020. [DOI: 10.1002/ange.202002797] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/19/2022]
Affiliation(s)
- Chun‐Lin Sun
- State Key Laboratory of Applied Organic Chemistry (SKLAOC)Key Laboratory of Special Function Materials and Structure Design (MOE)College of Chemistry and Chemical EngineeringLanzhou University Lanzhou 730000 P. R. China
| | - Jun Li
- MOE Key Laboratory of Material Physics and Chemistry under Extraordinary ConditionsSchool of Chemistry and Chemical EngineeringNorthwestern Polytechnical University Xi'an 710072 P. R. China
| | - Qi‐Wei Song
- State Key Laboratory of Applied Organic Chemistry (SKLAOC)Key Laboratory of Special Function Materials and Structure Design (MOE)College of Chemistry and Chemical EngineeringLanzhou University Lanzhou 730000 P. R. China
| | - Yu Ma
- MOE Key Laboratory of Material Physics and Chemistry under Extraordinary ConditionsSchool of Chemistry and Chemical EngineeringNorthwestern Polytechnical University Xi'an 710072 P. R. China
| | - Ze‐Qi Zhang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC)Key Laboratory of Special Function Materials and Structure Design (MOE)College of Chemistry and Chemical EngineeringLanzhou University Lanzhou 730000 P. R. China
| | - Jian‐Bo De
- Beijing Key Laboratory for Optical Materials and Photonic DevicesDepartment of ChemistryCapital Normal University Beijing 100048 P. R. China
| | - Qing Liao
- Beijing Key Laboratory for Optical Materials and Photonic DevicesDepartment of ChemistryCapital Normal University Beijing 100048 P. R. China
| | - Hongbing Fu
- Beijing Key Laboratory for Optical Materials and Photonic DevicesDepartment of ChemistryCapital Normal University Beijing 100048 P. R. China
- Tianjin Key Laboratory of Molecular Optoelectronic SciencesDepartment of ChemistryTianjin University, and CollaborativeInnovation Center of Chemical Science and Engineering (Tianjin) Tianjin 300072 P. R. China
| | - Jiannian Yao
- Beijing National Laboratory for Molecules Science (BNLMS)State Key Laboratory for Structural Chemistry of Unstable and Stable SpeciesKey Laboratory of PhotochemistryInstitute of ChemistryChinese Academy of Sciences Beijing 100190 P. R. China
- Tianjin Key Laboratory of Molecular Optoelectronic SciencesDepartment of ChemistryTianjin University, and CollaborativeInnovation Center of Chemical Science and Engineering (Tianjin) Tianjin 300072 P. R. China
| | - Hao‐Li Zhang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC)Key Laboratory of Special Function Materials and Structure Design (MOE)College of Chemistry and Chemical EngineeringLanzhou University Lanzhou 730000 P. R. China
- Tianjin Key Laboratory of Molecular Optoelectronic SciencesDepartment of ChemistryTianjin University, and CollaborativeInnovation Center of Chemical Science and Engineering (Tianjin) Tianjin 300072 P. R. China
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Ivanov SK, Kartashov YV, Maczewsky LJ, Szameit A, Konotop VV. Bragg solitons in topological Floquet insulators. OPTICS LETTERS 2020; 45:2271-2274. [PMID: 32287211 DOI: 10.1364/ol.390694] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/17/2020] [Accepted: 03/13/2020] [Indexed: 06/11/2023]
Abstract
We consider a topological Floquet insulator consisting of two honeycomb arrays of identical waveguides having opposite helicities. The interface between the arrays supports two distinct topological edge states, which can be resonantly coupled by additional weak longitudinal refractive index modulation with a period larger than the helix period. In the presence of Kerr nonlinearity, such coupled edge states enable topological Bragg solitons. Theory and examples of such solitons are presented.
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