Microstrip-antenna-coupled distributed feedback terahertz quantum-cascade lasers

By introducing coupled microstrip antennas on THz Distributed Feedback (DFB) Quantum Cascade Lasers (QCLs), the radiation efficiency of each feedback aperture is greatly enhanced. Single mode emission ∼3 THz from a 31-period antenna-coupled third-order DFB laser yields ∼4 times improvement in output...

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Bibliographic Details
Main Authors: Kao, Tsung-Yu (Author), Cai, Xiaowei (Author), Hu, Qing (Author), Reno, John L. (Author)
Other Authors: Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science (Contributor), Massachusetts Institute of Technology. Research Laboratory of Electronics (Contributor)
Format: Article
Language:English
Published: SPIE, 2021-12-20T15:32:04Z.
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Online Access:Get fulltext
LEADER 01950 am a22002053u 4500
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042 |a dc 
100 1 0 |a Kao, Tsung-Yu  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Research Laboratory of Electronics  |e contributor 
700 1 0 |a Cai, Xiaowei  |e author 
700 1 0 |a Hu, Qing  |e author 
700 1 0 |a Reno, John L.  |e author 
245 0 0 |a Microstrip-antenna-coupled distributed feedback terahertz quantum-cascade lasers 
260 |b SPIE,   |c 2021-12-20T15:32:04Z. 
856 |z Get fulltext  |u https://hdl.handle.net/1721.1/137750.2 
520 |a By introducing coupled microstrip antennas on THz Distributed Feedback (DFB) Quantum Cascade Lasers (QCLs), the radiation efficiency of each feedback aperture is greatly enhanced. Single mode emission ∼3 THz from a 31-period antenna-coupled third-order DFB laser yields ∼4 times improvement in output power comparing with a corrugated thirdorder device fabricated on the same gain medium. This 31-period device has ∼15×25° beam divergence and 4 mW pulsed power (4%) at 10 K with maximum lasing temperature (Tmax) at 134 K (pulsed). When phase matching condition is met, emissions from 81 apertures (4-mm long) are coherently combined to form a narrow beam with 12.5° divergence. Further experiment demonstrated the new device at 4 THz (25-period, ∼18 μm×1-mm long. The 4 THz device reaches >8 mW pulsed power (10%) at 12 K with Tmax109 K (pulsed) and >77 K (cw). The slope efficiency is 450 mW/A with 0.57% wall-plug. It is worth pointing out although the antennas would be excited differently, similar enhancement in out-coupling efficiency can also be observed in second-order surface-emitting THz DFB lasers. Begin the abstract two lines below author names and addresses.. © 2014 SPIE. 
546 |a en 
655 7 |a Article 
773 |t 10.1117/12.2036604