High power (130 mW) 40 GHz 1.55 μm mode-locked DBR lasers with integrated optical amplifiers J. Akbar, L. Hou, M. Haji,, M. J. Strain, P. Stolarz, J. H.

Slides:



Advertisements
Similar presentations
Sub-Picosecond Pulse Generation using Fast Saturable Absorption in AlGaInAs/InP Quantum Wells M. Haji, L. Hou, A. E. Kelly, R. G. Green, G. Mezosi, J.
Advertisements

Liverpool Group presentation 22/07/2009
Chapter 9. PN-junction diodes: Applications
2003/04/071 Characteristic of 850-nm InGaAs/AlGaAs Vertical-Cavity Surface-Emitting Lasers Master’s thesis of Yuni Chang Speaker:Han-Yi Chu National Changhua.
Optical sources Lecture 5.
AVANEX Livingston, Starlow Park, Livingston, EH54 8SF
About Omics Group OMICS GroupOMICS Group International through its Open Access Initiative is committed to make genuine and reliable contributions to the.
J. P. Reithmaier1,3, S. Höfling1, J. Seufert2, M. Fischer2, J
Mode locked laser array monolithically integrated with SOA and EA modulator L. Hou, M. Haji, A. E. Kelly, J. M. Arnold, A. C. Bryce.
Laser III Device Design & Materials Selection
School of Physics and Astronomy, University of Nottingham, Nottingham, NG7 2RD, UK. Electrically pumped terahertz SASER device using a weakly coupled AlAs/GaAs.
EE 230: Optical Fiber Communication Lecture 7 From the movie Warriors of the Net Optical Amplifiers-the Basics.
OEIC LAB National Cheng Kung University 1 Ching-Ting Lee Institute of Microelectronics, Department of Electrical Engineering, National Cheng Kung University.
Magneto-optical study of InP/InGaAs/InP quantum well B. Karmakar, A.P. Shah, M.R. Gokhale and B.M. Arora Tata Institute of Fundamental Research Mumbai,
Simulations of All-Optical Multiple-Input AND- Gate Based on Four Wave Mixing in a Single Semiconductor Optical Amplifier H. Le Minh, Z. Ghassemlooy, Wai.
Large Multilayer Diffraction Gratings: Coating Uniformity Senior Student: Erik Krous Project Advisor: Dr. Carmen Menoni Collaborators: Dr. D. Patel, Dr.
Fiber-Optic Communications James N. Downing. Chapter 5 Optical Sources and Transmitters.
Ch 6: Optical Sources Variety of sources Variety of sources LS considerations: LS considerations: Wavelength Wavelength  Output power Output power Modulation.
Thermally Deformable Mirrors: a new Adaptive Optics scheme for Advanced Gravitational Wave Interferometers Marie Kasprzack Laboratoire de l’Accélérateur.
Free-Space MEMS Tunable Optical Filter in (110) Silicon
Fiber Optic Light Sources
NA62 Gigatracker Working Group Meeting 2 February 2010 Massimiliano Fiorini CERN.
4/11/2006BAE Application of photodiodes A brief overview.
KM3NeTmeeting Pylos, Greece, April of 12 Mar van der Hoek et al. electronic department PROGRESS ON OPTICAL MODULATORS FOR KM3NeT Mar van der.
3/26/2003BAE of 10 Application of photodiodes A brief overview.
ECE 340 Lecture 27 P-N diode capacitance
Optical Sources
Lecture 6.
Waveguide High-Speed Circuits and Systems Laboratory B.M.Yu High-Speed Circuits and Systems Laboratory 1.
Controlling the dynamics time scale of a diode laser using filtered optical feedback. A.P.A. FISCHER, Laboratoire de Physique des Lasers, Universite Paris.
Lecture 7. Tunable Semiconductor Lasers What determines lasing frequency: Gain spectrum A function of temperature. Optical length of cavity Mirror reflectance.
Alan Kost Frontiers in Optics Tucson, AZ October 20, 2005 Monolithically Integrated Semiconductor Components for Coarse Wavelength Division Multiplexing.
Laser Diode Efficiencies
A High-Gain, Low-Noise, +6dBm PA in 90nm CMOS for 60-GHz Radio
Ultrafast Carrier Dynamics in Graphene M. Breusing, N. Severin, S. Eilers, J. Rabe and T. Elsässer Conclusion information about carrier distribution with10fs.
Folienvorlagen für Seminarvortrag. Novel laser concepts HR-mirror out coupling mirror disc cooling diode laser focusing optic diode laser focusing optic.
Itoh Lab. M1 Masataka YASUDA
Uni S T.E.Sale et al., HPSP 9, Sapporo 2000, paper 27P15. Gain-Cavity Alignment in Efficient Visible (660nm) VCSELs Studied Using High Pressure Techniques.
Min Hyeong KIM High-Speed Circuits and Systems Laboratory E.E. Engineering at YONSEI UNIVERITY
Optical sources Types of optical sources
Extending the principles of the Flygare: Towards a FT-THz spectrometer Rogier Braakman Chemistry & Chemical Engineering California Institute of Technology.
An H- stripping laser using commercial, diode-pumped Nd:YAG amplifiers Russell Wilcox Laser Stripping Workshop, April 11, 2011.
(a)luminescence (LED) (b)optical amplifiers (c)laser diodes.
P RESENTATION ON MONOLITHIC MICROWAVE INTEGRATED CIRCUITS PASSIVE COMPONENTS SUBMITTED BY:- AJAY KAUSHIK(088/ECE/09 ) NAMAN KUMAR(082/ECE/09 )
Yb:YAG Regenerative Amplifier for A1 Ground Laser Hut Rui Zhang ACCL Division V, RF-Gun Group Nov 20, 2015 SuperKEKB Injector Laser RF Gun Review.
Advanced laser and led structures, applications
3PNT – Advanced Laser Structures and Optical Communications (SJS)
Application of photodiodes
Optical Emitters and Receivers
Four wave mixing in submicron waveguides
L7 Lasers UConn ECE /27/2017 F. Jain
Integrated Semiconductor Modelocked Lasers
Single and dual wavelength Er:Yb double clad fiber lasers
OPTICAL SOURCE : Light Emitting Diodes (LEDs)
Optical Amplifier.
David Dahan and Gadi Eisenstein
Continued Advanced Semiconductor Lab.
High Power, Uncooled InGaAs Photodiodes with High Quantum Efficiency for 1.2 to 2.2 Micron Wavelength Coherent Lidars Shubhashish Datta and Abhay Joshi.
Simultaneous Wavelength Conversion and
Monolithically Integrated Mach-Zehnder Interferometer Wavelength Converter and Widely-Tunable Laser in InP Milan L. Mašanović, Vikrant Lal, Jonathon S.
Monolithically Integrated Mach-Zehnder Interferometer Wavelength Converter and Widely-Tunable Laser in InP Milan L. Mašanović, Vikrant Lal, Jonathon S.
Broadband Lateral Tapered Structures for Improved Bandwidth and Loss Characteristics for All-Optical Wavelength Converters Xuejin Yan, Joe Summers, Wei.
Broadband Lateral Tapered Structures for Improved Bandwidth and Loss Characteristics for All-Optical Wavelength Converters Xuejin Yan, Joe Summers, Wei.
External Modulation OEIC Wavelength Converters
Integration Platforms
Monolithically Integrated Mach-Zehnder Interferometer Wavelength Converter and Widely-Tunable Laser in InP Milan L. Mašanović, Vikrant Lal, Jonathon S.
Wavelength Converter Enhancements Using QWI
Broadband Lateral Tapered Structures for Improved Bandwidth and Loss Characteristics for All-Optical Wavelength Converters Xuejin Yan, Joe Summers, Wei.
Performance Optimization of AOWCs
Wave front and energy front
Presentation transcript:

High power (130 mW) 40 GHz 1.55 μm mode-locked DBR lasers with integrated optical amplifiers J. Akbar, L. Hou, M. Haji,, M. J. Strain, P. Stolarz, J. H. Marsh, A. C. Bryce and A. E. Kelly

Outline Motivation Wafer structure Material properties Device features & fabrication Device structure Device characterization Conclusions

Motivation Terahertz Generation OCDMA Non-linear optical effects RZ source Optical sampling Pumping

Wafer structure N cladding layerP cladding layerActive layer MQW decreased to 3 AlGaInAs/InP epitaxial structure with 3- quantum well active layer. A 160nm thick Far- field reduction layer (FRL) and 0.75 µm thick InP spacer layers were incorporated in the lower cladding to increase spot size while maintaining single mode operation substrate Farfield reduction layer

Material properties Increasing A/Γ increases saturation output power of SOAs FRL expands the near field towards n-cladding which results in reduced free carrier absorption. Increase in near field pattern results in low divergence angles which improves coupling with single mode fibers Higher gain saturation energy E sat is desirable in MLLs as it reduces pulse broadening in the gain section Increase in Esat can be achieved by: Increasing mode cross sectional area A. Decreasing optical confinement factor Γ Decreasing the differential gain dg/dN

Device features Optimised 3QW AlGaInAs/InP material Planarisation using Hydrogen Silsesquioxane (HSQ) Avoids breaks in p-contact metallization Simulated results shows reduced optical losses in the DBRs Surface-etched DBR: Require only a single epitaxial growth step Simultaneously fabricated with the ridge waveguide Al-containing active layers can be used without the risk of oxidization 1mm long curved SOA with tilt angle of 10 degrees is fabricated

Device Structure Cavity length = 1125 μm DBR length = 150 μm SOA length= 1000 μm SOA output tilt angle= 10˚ Gratings period (Λ)= 734 nm Slot width = 180 nm DBR effective length = 70 μm SA Gain DBR SOA Slot 180nm

Power measurements Power measured from SA facet: DBR current fixed at 5mA, SOA is floating Average output power in mode locked conditions from SA side is ~ 28mW

Power measurements Power measured from SOA end: DBR current fixed at 5mA, SOA current 250mA Average output Power in mode locked conditions from SOA end is ~ 130mW

Power measurements Power measured from SOA end: DBR current 5mA, SA reverse voltage -4V DBR 5mA, Gain 250mA

LI & optical spectrum of SOA SA, Gain and DBR floating, SOA biased Low amplitude of modulations in the optical spectrum indicates that effective reflectivity from the tilted facet is sufficiently reduced. Small peaks in the optical spectrum is due to DBR stop band.

Mode locking results Gain current 200mA, SOA current 250mA, SA -4V ʋ = 1.3 MHz Δt = 3.3 ps Minimum pulse width of 3.3ps assuming Gaussian fit. RF peak is ~45dB above the noise floor with RF linewidth of 1.3MHz ps

Mode locking results Gain current 220mA SOA current 250mA Δλ=1.14nm FWHM 1.9 nm

Output peak power and TBP SOA current = 250mA, SA = -4V Gain current 220mA, V SA = -4V With increase in SOA current, output peak power also increases whilst TBP is constant at around This shows near transform limited pulses over wide range of SOA currents.

Farfield measurements Devices with integrated 1mm long SOA Vertical direction Horizontal direction Farfield-3D view Farfield-2D view

Conclusions Mode-Locked DBR Laser with integrated SOA : Surface etched DBR mode locked laser Novel epitaxial structure with optimized 3 QW active region and FRL High average output power 130mW and peak power > 1W in mode locked operation Integration of SOA increases output power by a factor of ~ 5. Minimum pulse width of 3.3 ps with 3 dB optical spectral bandwidth of 1.14 nm and TBP of 0.45 assuming Gaussian shaped pulses Reduced divergence angle Output peak power can be increased by further increasing the mode size or increasing the reflection bandwidth of DBR

Acknowledgements The technical staff of JWNC at the University of Glasgow This work is a part of EPSRC EP/E065112/1 High Power, High Frequency Mode-locked Semiconductor Lasers and funded by Higher education commission of Pakistan.EP/E065112/1 HIGHER EDUCATION COMMISSION Islamabad (Pakistan)