Longitudinal optical (LO) and LO-like phonon resonant mid-infrared radiation emission and absorption by surface micro-structures on III-nitrides

被引:0
作者
Ishitani, Yoshihiro [1 ]
Lin, Bojin [1 ]
Aye, Hnin Lai Lai [1 ]
Yoshikawa, Daiki [1 ]
Miyake, Hideto [2 ]
Ueno, Kohei [3 ]
Fujioka, Hiroshi [3 ]
机构
[1] Grad Sch Elect & Elect Engn, 1-33 Yayoicho,Inage Ku, Chiba 2638522, Japan
[2] Mie Univ, Grad Sch Engn, 1577 Kurimamachiya, Tsu, Mie 5148507, Japan
[3] Univ Tokyo, Inst Ind Sci, 4-6-1 Komaba,Meguro Ku, Tokyo 1538505, Japan
来源
GALLIUM NITRIDE MATERIALS AND DEVICES XIX | 2024年 / 12886卷
关键词
Longitudinal optical phonon; thermal emission; mid-infrared radiation; surface microstructures; III-nitrides; phonon coherence; CARRIER; LIGHT;
D O I
10.1117/12.3000696
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Longitudinal optical-like phonon resonant mid-infrared emission (LORE) and absorption peaks of micro-surface line and space structures of metallic material plates on GaN wafers are observed at 500 - 630 K. The emission peak energy is located in a range of 670 - 730 cm(-1) for GaN, which is lower than the LO-phonon energy of approximately 730 cm(-1) at 630 K. This feature is contrasted with that of the LO-phonon resonant emission from the Au.GaAs microstructures resonating with the LO phonon. The emission mechanism is clarified using a structure of n(++)-GaN with an electron density of 1.1020 cm(-3) as a metallic material. These emission lines have another notable feature, i.e., the observed peak energies are independent of the polar emission angle, unlike the emissions by surface phonon polaritons showing a significant directive nature of peak energies. The present results show that each peak energy in the emission spectrum is positioned at the zero-point of the real part of the dielectric function comprising the components of the transverse optical phonon and other electric dipoles induced by the LO-like modes, excluding the target mode. This type of emission is also obtained for the structures of AlxGa1-xN films. These results suggest the feasibility of high-efficiency emission in a range of 670 - 900 cm(-1) when the devices are positioned in a cavity with high reflectivity of blackbody-like radiation.
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页数:9
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