1.Division of Quantum Materials and Devices, Beijing Academy of Quantum Information Sciences, Beijing 100193, China
2.Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
3.School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
4.Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
Lijun Wang (ljwang@semi.ac.cn)
Quanyong Lu (luqy@baqis.ac.cn)
收稿日期:2024-02-26,
修回日期:2024-07-30,
录用日期:2024-08-06,
网络出版日期:2024-08-16,
纸质出版日期:2024-10-31
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High brightness terahertz quantum cascade laser with near-diffraction-limited Gaussian beam[J]. LSA, 2024,13(10):2124-2130.
Li, R. S. et al. High brightness terahertz quantum cascade laser with near-diffraction-limited Gaussian beam. Light: Science & Applications, 13, 2124-2430 (2024).
High brightness terahertz quantum cascade laser with near-diffraction-limited Gaussian beam[J]. LSA, 2024,13(10):2124-2130. DOI: 10.1038/s41377-024-01567-2.
Li, R. S. et al. High brightness terahertz quantum cascade laser with near-diffraction-limited Gaussian beam. Light: Science & Applications, 13, 2124-2430 (2024). DOI: 10.1038/s41377-024-01567-2.
High-power terahertz (THz) quantum cascade laser
as an emerging THz solid-state radiation source
is attracting attention for numerous applications including medicine
sensing
and communication. However
due to the sub-wavelength confinement of the waveguide structure
direct beam brightness upscaling with device area remains elusive due to several mode competition and external optical lens is normally used to enhance the THz beam brightness. Here
we propose a metallic THz photonic crystal resonator with a phase-engineered design for single mode surface emission over a broad area. The quantum cascade surface-emitting laser is capable of delivering an output peak power over 185 mW with a narrow beam divergence of 4.4° × 4.4° at 3.88 THz. A high beam brightness of 1.6 × 10
7
W sr
−1
m
−2
with near-diffraction-limited M
2
factors of 1.4 in both vertical and lateral directions is achieved from a lar
ge device area of 1.6 × 1.6 mm
2
without using any optical lenses. The adjustable phase shift between the lattices enables a stable and high-intensity surface emission over a broad device area
which makes it an ideal light extractor for large-scale THz emitters. Our research paves the way to high brightness solid-state THz lasers and facilitates new applications in standoff THz imaging
detection
and diagnosis.
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