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General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Downloaded from orbit.dtu.dk on: Sep 07, 2021 Doppler wind lidar using a MOPA semiconductor laser at stable single-frequency operation Rodrigo, Peter John; Pedersen, Christian Published in: Conference abstract series, CLEO/Europe - EQEC Link to article, DOI: 10.1109/CLEOE-EQEC.2009.5196300 Publication date: 2009 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Rodrigo, P. J., & Pedersen, C. (2009). Doppler wind lidar using a MOPA semiconductor laser at stable single- frequency operation. In Conference abstract series, CLEO/Europe - EQEC (pp. 1-1). IEEE. https://doi.org/10.1109/CLEOE-EQEC.2009.5196300
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Page 1: Doppler wind lidar using a MOPA semiconductor laser at stable … · Doppler wind lidar using a MOPA semiconductor laser at stable single-frequency operation Rodrigo, Peter John;

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Users may download and print one copy of any publication from the public portal for the purpose of private study or research.

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You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim.

Downloaded from orbit.dtu.dk on: Sep 07, 2021

Doppler wind lidar using a MOPA semiconductor laser at stable single-frequencyoperation

Rodrigo, Peter John; Pedersen, Christian

Published in:Conference abstract series, CLEO/Europe - EQEC

Link to article, DOI:10.1109/CLEOE-EQEC.2009.5196300

Publication date:2009

Document VersionPublisher's PDF, also known as Version of record

Link back to DTU Orbit

Citation (APA):Rodrigo, P. J., & Pedersen, C. (2009). Doppler wind lidar using a MOPA semiconductor laser at stable single-frequency operation. In Conference abstract series, CLEO/Europe - EQEC (pp. 1-1). IEEE.https://doi.org/10.1109/CLEOE-EQEC.2009.5196300

Page 2: Doppler wind lidar using a MOPA semiconductor laser at stable … · Doppler wind lidar using a MOPA semiconductor laser at stable single-frequency operation Rodrigo, Peter John;

Doppler wind Iidar using a MOPA semiconductor laser at stablesingle-frequency operation

Peter John Rodrigo and Christian PedersenDTU Fotonik, TechnicalUniversity ofDenmark, Frederiksborgvej 399, DK-4000Roskilde, Denmark

Our group has recently demonstrated that a compact master-oscillator power-amplifier semiconductor laser(MOPA-SL) is a good candidate for a coherent light source (operating at 1550 nm) in a Doppler wind Lidar [I]. TheMOPA-SL requires two injection currents: IOFB for the distributed-feedback (DFB) laser section (master oscillator) andlAMP for the tapered amplifier section. For our laser, the specified maximum current values are 0.7 A and 4.0 A for IOFBand lAMP, respectively. Figure I(a) shows the measurement of CW output power of the MOPA-SL versus lAMP for threedifferent values ofIOFB = 400,500, and 600 rnA. Our measurements were taken at 19 DC set temperature. The L-I curveshows that the output power linearly increases with lAMP and reaches an ample I W level. Although the MOPA-SL hasbeen proven capable of producing single-frequency CW output beam, stable operation at this spectral condition has alsobeen known to highly depend on the drive currents to the laser [2]. It is therefore important to identify pockets ofstability in the IOFB-lAMP""Ts (Ts = laser set temperature) space where lasting single-frequency operation is achieved. At achosen set temperature Ts = 19 DC, we searched for combinations of (lOFB, lAMP) where the laser operates stably at single­frequency. This was done by observing the spectral characteristic of the laser using an optical spectrum analyzer (OSA,ANDO AQ63 15) at different drive current combinations. The resolution of the OSA used is 0.05 nm. Depending on thedrive currents, single-frequency or multi-frequency operations of the laser may occur as shown in Fig I(b).Furthermore, hysteretic mode-hops between single-frequency regimes can occur at higher values of lAMP. When usingthe laser for a Doppler wind Lidar application, a combination of (loFB, lAMP) which is close to the center of an identifiedstable single-frequency regime is used . For the MOPA-SL unit that we use in our Lidar, we typically use (lOFB = 0.5 A,lAMP = 3.0 A) at Ts = 19 DC. These current settings for the laser result in a highly stable Lidar as shown by a 5-day longcontinuous measurement of the Doppler shift produced by a constantly rotating diffusely reflecting target (Fig. 2).

(a) (b)1I

0.8 ![ I lAMP= 3.0 A; T = 19.0 deg C; Ando-OSA AAres" = 0.05 nm lAMP = 4.0 A; Ts = 19.0 deg C; Ando-OSA M ,es = 0.05 nm

lD 0 lD 0

~ 0.6 t "'- IOFB - 500.0 rnA "'- IDFB= 498.3 rnA0 :;; -10 :;; -100- t ;:: ;::'5 0 0

0.4 + 600mA0- -20 0- -20

So • S S::l So -30 c, -300 • 500mA:J S I'0.2 • .. 400mA 0

-400

-40

" LJ \ " _ / \.• > ."~ -sc 1ii -scO· Qi l---',- I I i I I 1"-'-

Qi I I I 1'-'" '"0 1 2 3 4 -60 -60

1 5~ 1 5~1 5Q l~41~ 1~81 5~ 1~21 ~4 1~61 5M 1~8 1~O l~2 1~1~6 15~15~1~1~15$1~

Amplifier Current [AI Wavelength [nm] Wavelength [nm)

Fig. 1. Characterization of the MOPA-SL's (a) output powerand (b) spectralpropertiesfor differentdrivecurrents.

12.8 r--------------------------,

N 12.4 +- - - - - - - - - - - - - - - - - - - - - - - ----l:l:

~..~ 12 r------".-------""-------!1111--+..Q.c,oc 11.6 +- - - - - - - - - - - - - - - - - - - - - - - ----l

8070605040302010

11.2 !----~--~-------------~--------'

ohrs. (each data pt is 10 min ave)

Fig. 2. Lidar-measured to-minute averageDopplershift (-12 MHz) producedby a hard-targetrotatingat constantrate. Standarddeviations of<0.1 MHz for any data point is indicative of the high stabilityof the laser sourceover an 80-hourperiod.

References[1] R. S. Hansenand C. Pedersen, "All semiconductor laser Doppleranemometer at 1.5511m," Opt. Express 16, 18288(2008).[2] A Egan,et aI., "Dynamic Instabilities in MasterOscillatorPowerAmplifierSemiconductor Lasers," IEEEJ. QuantumElectron. 34,166 (1998).

978-1-4244-4080-1/09/$25.00 @2009 IEEE

Authorized licensed use limited to: Danmarks Tekniske Informationscenter. Downloaded on October 28, 2009 at 09:15 from IEEE Xplore. Restrictions apply.


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