Dual Laser Indium Phosphide Photonic Integrated Circuit for Integrated Path Differential Absorption Lidar

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Dual_Laser_Indium_Phosphide_Photonic_Integrated_Circuit_for_Integrated_Path_Differential_Absorption_Lidar.pdf (3.81 MB)

Links to Files

https://ieeexplore.ieee.org/document/9462382

Permanent Link

https://doi.org/10.1109/JSTQE.2021.3091662
 http://hdl.handle.net/11603/23956

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UMBC Center for Space Sciences and Technology (CSST) / Center for Research and Exploration in Space Sciences & Technology II (CRSST II)
UMBC Faculty Collection
UMBC Physics Department

Author/Creator

Author/Creator ORCID

https://orcid.org/0000-0002-7204-2512

Date

2021-06-22

Type of Work

journal articles
Text

Department

Program

Citation of Original Publication

J. Fridlander et al., "Dual Laser Indium Phosphide Photonic Integrated Circuit for Integrated Path Differential Absorption Lidar," in IEEE Journal of Selected Topics in Quantum Electronics, vol. 28, no. 1, pp. 1-8, Jan.-Feb. 2022, Art no. 6100208, doi: 10.1109/JSTQE.2021.3091662.

Rights

This work was written as part of one of the author's official duties as an Employee of the United States Government and is therefore a work of the United States Government. In accordance with 17 U.S.C. 105, no copyright protection is available for such wo
Public Domain Mark 1.0

Subjects

Abstract

An indium phosphide photonic integrated circuit (PIC) was demonstrated for integrated path differential absorption lidar of atmospheric carbon dioxide (CO 2 ). The PIC consists of two widely tunable sampled grating distributed Bragg reflector (SGDBR) lasers, directional couplers, a phase modulator, a photodiode, and semiconductor optical amplifiers (SOAs). One SGDBR laser, the leader, is locked to the center of an absorption line at 1572.335 nm using the on-chip phase modulator and a bench-top CO 2 Herriott reference cell. The other SGDBR laser, the follower, is stepped in frequency over ±15 GHz around 1572.335 nm to scan the target CO 2 absorption line. The follower laser is offset locked to the leader laser with an optical phase lock loop. An SOA after the follower laser generates a pulse at each frequency step to create a train of pulses that samples the target CO 2 absorption line. The PIC components and subsystem are characterized and evaluated based on target performance requirements. The leader laser demonstrated a 236-fold improvement in frequency stability standard deviation when locked compared to free running and the follower laser frequency stability standard deviation compared to the leader laser was 37.6 KHz at a 2 GHz programmed offset.