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Highly efficient optoelectronic devices of ultrasmall sizes are demanded as building blocks of next-generation integrated circuits, where tunable color enhances the feasibility of various applications. Here, we realize tunable multicolor nanolasers using disk-shaped axial heterostructures composed of III-nitride materials (GaN/InGaN/GaN), leveraging the optical confinement effect and active waveguiding. In heterostructure nanodisks, the development of exciton-polariton induces unique features near the resonance regime, and the formation of whispering-gallery modes facilitates optical gain processes for the polaritonic lasing of GaN. Likewise, the polaritonic lasing of InGaN emerges, although the small gain volume in the quantum well structure hinders strong amplification. Notably, the characteristics of lasing differ between GaN and InGaN, suggesting a distinctive polariton behavior in quantum well structures. The alloyed systems enable tunable laser colors in the visible region, while whispering-gallery modes afford independent control of lasing. Therefore, we establish tunable dual-color polariton nanolasers using heterostructure disks for the first time, achieving nanophotonic devices that take advantage of the optical confinement effect and active waveguiding.
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http://dx.doi.org/10.1039/d5nr02469b | DOI Listing |
Nanoscale
September 2025
Department of Chemistry, Kyung Hee University, Seoul 02447, Korea.
Highly efficient optoelectronic devices of ultrasmall sizes are demanded as building blocks of next-generation integrated circuits, where tunable color enhances the feasibility of various applications. Here, we realize tunable multicolor nanolasers using disk-shaped axial heterostructures composed of III-nitride materials (GaN/InGaN/GaN), leveraging the optical confinement effect and active waveguiding. In heterostructure nanodisks, the development of exciton-polariton induces unique features near the resonance regime, and the formation of whispering-gallery modes facilitates optical gain processes for the polaritonic lasing of GaN.
View Article and Find Full Text PDFSensors (Basel)
August 2025
Consiglio Nazionale delle Ricerche, Istituto Nazionale di Ottica (INO), Via Campi Flegrei, 34-Comprensorio A. Olivetti, 80078 Pozzuoli, Italy.
Whispering-gallery-mode (WGM) microresonators are amongst the most promising optical sensors for detecting bio-chemical targets. A number of laser interrogation methods have been proposed and demonstrated over the last decade, based on scattering and absorption losses or resonance splitting and shift, harnessing the high-quality factor and ultra-small volume of WGMs. Actually, regardless of the sensitivity enhancement, their practical sensing operation may be hampered by the complexity of coupling devices as well as the signalprocessing required to extract the WGM response.
View Article and Find Full Text PDFWe study whispering gallery modes (WGMs) of a ring resonator formed by a highly elliptical two-mode fiber. By imparting the twist to the fiber, one can make this system's topology similar to a Möbius stripe's topology. We show that WGMs of such a Möbius ring resonator (MRR) carry intrinsic orbital angular momentum (OAM).
View Article and Find Full Text PDFPropagation of whispering gallery modes in surface nanoscale axial photonics (SNAP) microresonators, fabricated at the optical fiber surface, is commonly described by a one-dimensional wave equation, resembling the Schrödinger equation, where the fiber cutoff frequency (CF), varying along the fiber length plays the role of potential and the light frequency plays the role of energy. Of particular importance for applications including frequency comb generation, frequency conversion, and signal processing are SNAP microresonators with constant free spectrum range (FSR). Here, we note that, in addition to CF potentials with a globally constant FSR, the potentials having constant FSR confined within a specific spectral region may be sufficient or, in certain cases, preferable for a range of applications.
View Article and Find Full Text PDFHigh whispering gallery mode (WGM) optical resonators can achieve a high nonlinear frequency conversion efficiency with quite low input laser intensity. Third harmonic generation (THG) in a WGM resonator requires phase-matching which is conventionally accomplished by careful engineering of the dispersion of the cavity modes. Input laser power-induced temperature-dependent dispersion is often used to additionally compensate the residual phase mismatch.
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