Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation

When a fraction of the light reflected by an external cavity re-enters the laser cavity, both the amplitude and the frequency of the lasing field can be modulated. This phenomenon is called the self-mixing effect (SME). A self-mixing laser diode (SM-LD) is a sensor using the SME. Usually, such LDs o...

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Main Authors: Bin Liu, Yanguang Yu, Jiangtao Xi, Yuanlong Fan, Qinghua Guo, Jun Tong, Roger A. Lewis
Format: Article
Language:English
Published: MDPI AG 2016-09-01
Series:Sensors
Subjects:
Online Access:http://www.mdpi.com/1424-8220/16/9/1546
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spelling doaj-81d0eac0d5bc4ebd9d5664e6f19559d42020-11-24T21:19:10ZengMDPI AGSensors1424-82202016-09-01169154610.3390/s16091546s16091546Features of a Self-Mixing Laser Diode Operating Near Relaxation OscillationBin Liu0Yanguang Yu1Jiangtao Xi2Yuanlong Fan3Qinghua Guo4Jun Tong5Roger A. Lewis6School of Electrical, Computer and Telecommunications Engineering, University of Wollongong, Northfields Ave, Wollongong, NSW 2522, AustraliaSchool of Electrical, Computer and Telecommunications Engineering, University of Wollongong, Northfields Ave, Wollongong, NSW 2522, AustraliaSchool of Electrical, Computer and Telecommunications Engineering, University of Wollongong, Northfields Ave, Wollongong, NSW 2522, AustraliaSchool of Physics, University of Wollongong, Wollongong, NSW 2522, AustraliaSchool of Electrical, Computer and Telecommunications Engineering, University of Wollongong, Northfields Ave, Wollongong, NSW 2522, AustraliaSchool of Electrical, Computer and Telecommunications Engineering, University of Wollongong, Northfields Ave, Wollongong, NSW 2522, AustraliaSchool of Physics, University of Wollongong, Wollongong, NSW 2522, AustraliaWhen a fraction of the light reflected by an external cavity re-enters the laser cavity, both the amplitude and the frequency of the lasing field can be modulated. This phenomenon is called the self-mixing effect (SME). A self-mixing laser diode (SM-LD) is a sensor using the SME. Usually, such LDs operate below the stability boundary where no relaxation oscillation happens. The boundary is determined by the operation condition including the injection current, optical feedback strength and external cavity length. This paper discovers the features of an SM-LD where the LD operates beyond the stability boundary, that is, near the relaxation oscillation (RO) status. We call the signals from such a SM-LD as RO-SM signals to differentiate them from the conventional SM signals reported in the literature. Firstly, simulations are made based on the well-known Lang and Kobayashi (L-K) equations. Then the experiments are conducted on different LDs to verify the simulation results. It shows that a RO-SM signal exhibits high frequency oscillation with its amplitude modulated by a slow time varying envelop which corresponds to the movement of the external target. The envelope has same fringe structure (half-wavelength displacement resolution) with the conventional SM signals. However, the amplitudes of the RO-SM signals are much higher compared to conventional SM signals. The results presented reveal that an SM-LD operating near the RO has potential for achieving sensing with improved sensitivity.http://www.mdpi.com/1424-8220/16/9/1546self-mixing effectlaser dioderelaxation oscillationstability boundary
collection DOAJ
language English
format Article
sources DOAJ
author Bin Liu
Yanguang Yu
Jiangtao Xi
Yuanlong Fan
Qinghua Guo
Jun Tong
Roger A. Lewis
spellingShingle Bin Liu
Yanguang Yu
Jiangtao Xi
Yuanlong Fan
Qinghua Guo
Jun Tong
Roger A. Lewis
Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
Sensors
self-mixing effect
laser diode
relaxation oscillation
stability boundary
author_facet Bin Liu
Yanguang Yu
Jiangtao Xi
Yuanlong Fan
Qinghua Guo
Jun Tong
Roger A. Lewis
author_sort Bin Liu
title Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
title_short Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
title_full Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
title_fullStr Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
title_full_unstemmed Features of a Self-Mixing Laser Diode Operating Near Relaxation Oscillation
title_sort features of a self-mixing laser diode operating near relaxation oscillation
publisher MDPI AG
series Sensors
issn 1424-8220
publishDate 2016-09-01
description When a fraction of the light reflected by an external cavity re-enters the laser cavity, both the amplitude and the frequency of the lasing field can be modulated. This phenomenon is called the self-mixing effect (SME). A self-mixing laser diode (SM-LD) is a sensor using the SME. Usually, such LDs operate below the stability boundary where no relaxation oscillation happens. The boundary is determined by the operation condition including the injection current, optical feedback strength and external cavity length. This paper discovers the features of an SM-LD where the LD operates beyond the stability boundary, that is, near the relaxation oscillation (RO) status. We call the signals from such a SM-LD as RO-SM signals to differentiate them from the conventional SM signals reported in the literature. Firstly, simulations are made based on the well-known Lang and Kobayashi (L-K) equations. Then the experiments are conducted on different LDs to verify the simulation results. It shows that a RO-SM signal exhibits high frequency oscillation with its amplitude modulated by a slow time varying envelop which corresponds to the movement of the external target. The envelope has same fringe structure (half-wavelength displacement resolution) with the conventional SM signals. However, the amplitudes of the RO-SM signals are much higher compared to conventional SM signals. The results presented reveal that an SM-LD operating near the RO has potential for achieving sensing with improved sensitivity.
topic self-mixing effect
laser diode
relaxation oscillation
stability boundary
url http://www.mdpi.com/1424-8220/16/9/1546
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