High Power Compact Fiber Chirped Pulse Amplifiers at 1558-nm using Er/Yb LMA Fibers and Chirped Volume Bragg Grating Compressors

Similar documents
Large-aperture chirped volume Bragg grating based fiber CPA system

1 kw, 15!J linearly polarized fiber laser operating at 977 nm

Development of high average power fiber lasers for advanced accelerators

Fiber Lasers for EUV Lithography

Recent Progress in Active Fiber Designs and Monolithic High Power Fiber Laser Devices. Kanishka Tankala, Adrian Carter and Bryce Samson

C. J. S. de Matos and J. R. Taylor. Femtosecond Optics Group, Imperial College, Prince Consort Road, London SW7 2BW, UK

High peak power pulsed single-mode linearly polarized LMA fiber amplifier and Q-switch laser

Lasers à fibres ns et ps de forte puissance. Francois SALIN EOLITE systems

High Power Femtosecond Fiber Chirped Pulse Amplification System for High Speed Micromachining

Fiber lasers: The next generation

Fiber Laser Chirped Pulse Amplifier

Simultaneous pulse amplification and compression in all-fiber-integrated pre-chirped large-mode-area Er-doped fiber amplifier

Designing for Femtosecond Pulses

Directly Chirped Laser Source for Chirped Pulse Amplification

Integrated disruptive components for 2µm fibre Lasers ISLA. 2 µm Sub-Picosecond Fiber Lasers

Progress in ultrafast Cr:ZnSe Lasers. Evgueni Slobodtchikov, Peter Moulton

Ring cavity tunable fiber laser with external transversely chirped Bragg grating

Characterization of Chirped volume bragg grating (CVBG)

Development of High-peak Power Yb-doped Fiber Laser in Large Core Fiber

Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm

ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating

Development of scalable laser technology for EUVL applications

High-peak power laser system used in Yb doped LMA fiber

Dispersion and Ultrashort Pulses II

Survey Report: Laser R&D

HIGH POWER LASERS FOR 3 RD GENERATION GRAVITATIONAL WAVE DETECTORS

Bragg and fiber gratings. Mikko Saarinen

MULTI-STAGE YTTERBIUM FIBER-AMPLIFIER SEEDED BY A GAIN-SWITCHED LASER DIODE

Photonic time-stretching of 102 GHz millimeter waves using 1.55 µm nonlinear optic polymer EO modulators

High Power Fiber lasers and Amplifiers: A tutorial overview

Analysis of Self Phase Modulation Fiber nonlinearity in Optical Transmission System with Dispersion

156 micro-j ultrafast Thulium-doped fiber laser

Development of near and mid-ir ultrashort pulse laser systems at Q-Peak. Evgueni Slobodtchikov Q-Peak, Inc.

High-gain Er-doped fiber amplifier generating eye-safe MW peak-power, mj-energy pulses

STUDY OF CHIRPED PULSE COMPRESSION IN OPTICAL FIBER FOR ALL FIBER CPA SYSTEM

Chirped Pulse Amplification

X-CAN. A coherent amplification network of femtosecond fiber amplifiers

1550 nm Programmable Picosecond Laser, PM

High-power semiconductor lasers for applications requiring GHz linewidth source

Improving efficiency of CO 2

High-Power, Passively Q-switched Microlaser - Power Amplifier System

ABSTRACT 1. INTRODUCTION

High average power picosecond pulse generation from a thulium-doped all-fiber MOPA system

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression

High Power and Energy Femtosecond Lasers

Sub-300 fs, 0.5 mj pulse at 1kHz from Ho:YLF amplifier and Kagome pulse compression

Photonics (OPTI 510R 2017) - Final exam. (May 8, 10:30am-12:30pm, R307)

Rogério Nogueira Instituto de Telecomunicações Pólo de Aveiro Departamento de Física Universidade de Aveiro

Longitudinal mode selection in laser cavity by moiré volume Bragg grating

J-KAREN-P Session 1, 10:00 10:

Pulse energy vs. Repetition rate

High-Power Femtosecond Lasers

Laser systems for science instruments

How to build an Er:fiber femtosecond laser

New generation of high average power industry grade ultrafast Ytterbium fiber lasers

Dr. Rüdiger Paschotta RP Photonics Consulting GmbH. Competence Area: Fiber Devices

Experimental Physics. Experiment C & D: Pulsed Laser & Dye Laser. Course: FY12. Project: The Pulsed Laser. Done by: Wael Al-Assadi & Irvin Mangwiza

Ultrafast instrumentation (No Alignment!)

Pulse stretching and compressing using grating pairs

Chirped Bragg Grating Dispersion Compensation in Dense Wavelength Division Multiplexing Optical Long-Haul Networks

The Realization of Ultra-Short Laser Sources. with Very High Intensity

Diode-pumped Yb:SSO chirped pulse amplifier with 1 ps pulse duration

Development of Nano Second Pulsed Lasers Using Polarization Maintaining Fibers

Ultrafast Lasers with Radial and Azimuthal Polarizations for Highefficiency. Applications

Thermal tuning of volume Bragg gratings for high power spectral beam combining

GOOCH & HOUSEGO NOVEL OPTICAL COMPONENTS FOR THE IR

Developments in new high power fiber lasers and ultrafast lasers

Thermal treatment method for tuning the lasing wavelength of a DFB fiber laser using coil heaters

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband

Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania

80 khz repetition rate high power fiber amplifier flat-top pulse pumped OPCPA based on BIB 3 O 6

DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE

A New Concept in Picosecond Lasers

DWDM FILTERS; DESIGN AND IMPLEMENTATION

External cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT

INGAAS FAST PIN (RF) AMPLIFIED PHOTODETECTORS

Pulsed 1064nm / 1030nm Narrow Bandwidth FBG High Power Laser Diode Module

Dr. Monir Hossen ECE, KUET

The Development of a High Quality and a High Peak Power Pulsed Fiber Laser With a Flexible Tunability of the Pulse Width

Cooled 10pin butterfly 980nm Pump Laser Module. Applications

Multi-MW peak power, single transverse mode operation of a 100 micron core diameter, Yb-doped photonic crystal rod amplifier

Generation mode-locked square-wave pulse based on reverse. saturable absorption effect in graded index multimode fiber

Synchronization In Advanced Optical Communications

3550 Aberdeen Ave SE, Kirtland AFB, NM 87117, USA ABSTRACT 1. INTRODUCTION

Photonic Crystal Fiber Interfacing. In partnership with

A new picosecond Laser pulse generation method.

Mitigation of Self-Pulsing in High Power Pulsed Fiber Lasers

Fiber Optic Communications

Survey Report: Laser R&D

Evaluation Kit Picosecond Fiber Laser PSFL1030 (REV )

Outline. Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements

Introduction Compact 0.56 PW laser system Scalability to multi-petawatt power Conclusion

High Power Thin Disk Lasers. Dr. Adolf Giesen. German Aerospace Center. Institute of Technical Physics. Folie 1. Institute of Technical Physics

Evaluation Kit Picosecond Fiber Laser PSFL1030

83 W, 3.1 MHz, square-shaped, 1 ns-pulsed all-fiber-integrated laser for micromachining

Advanced seeders for fiber lasers - IFLA. 23 June. 2014

Single-Frequency, 2-cm, Yb-Doped Silica-Fiber Laser

High peak power singlefrequency. applications

Ultrafast Laser Solutions for Microprocessing

DLA Laser Working Group Close Out Report

Transcription:

High Power Compact Fiber Chirped Pulse Amplifiers at 1558-nm using Er/Yb LMA Fibers and Chirped Volume Bragg Grating Compressors Ming-Yuan Cheng, Almantas Galvanauskas University of Michigan Vadim Smirnov, Emily Flecher, Leonid Glebov College of Optics and Photonics/CREOL, University of Central Florida J. Farroni, K. Tankala, A. Carter,, B. Samson, Machewirth, N. Jacobson Nufern A. Sanchez AFRL/DELO, Kirtland AFB

Outline Introduction Chirped Volume Bragg Grating (CVBG) stretchers/compressors Compact high power fiber CPA at 1558-nm based on CVBG High power Er/Yb fiber amplifiers CVBG power handling characteristics PM and non-pm CVBG compressor configurations Summary

Motivation Current Fiber CPA techniques: Diffraction-grating compressors Large and complex Fiber Bragg grating compressors Hollow-core PCF compressors Low pulse energies (< 1-µJ) New CVBG pulse compression technology: Compact & robust/simple alignment Potential for both high-power and high pulse energy scaling

Chirped Volume Bragg Grating (CVBG) Stretcher/Compressor PTR (Photo-Thermo-Refractive) glass λ Rely on Bragg reflection B - Same as FBG mm-large apertures - Main difference from FBG = nλ( z)

Chirped Volume Bragg Grating Potentially achievable characteristics: Long stretched pulses 0.1 1 ns Demonstrated: (1-cm 10-cm long CVGB) Stretched pulses 80-100ps > mj pulse energies (both extractable and compressible) High power/energy handling capacity High efficiency (>90 %) Compact and robust Reciprocal stretching and recompression High average power (15W recompressed)

Comparison between Conventional and CVBG Compressors Diffraction grating Compressor cavity ~40-cm Conventional Grating Compressor Chirped Volume Grating Compressor

PM-Fiber CPA Set-up 18/50 Er/Yb PM DC Fiber Amplifier 10m SMF-1 SM EDFA Dispersion compensator XYZ XYZ modelocked fiber laser PBS PBS Pump diode XYZ λ/ λ/4 λ/4 CVBG λ/ XYZ PM VCBG compressor

Amplified 1558-nm signal 15 amplified signal (W) 10 5 0 0 0 40 60 80 coupled pump power (W)

Grating reflectivity is power independent 100 grating reflectivity (%) 80 60 40 0 1-mm radius beam in the CVBG compressor 0 0 5 10 15 0 input power (W)

Recompressed Pulse (@ 6-W recompressed power) 1. Measured autocorrelation BW calculated autocorrelation Amplitude,a.u. 0.8 0.4 Reciprocal stretching/recompression 1.1-ps pulses 0-6 - 6 Time delay, ps

Non-PM Fiber CPA Set-up 5/300 Er/Yb DC Fiber Amplifier 0m SMF-1 SM EDFA Dispersion compensator XYZ XYZ modelocked fiber laser Pump diode XYZ Non-PM VCBG compressor CVBG λ/4 λ/ XYZ 15W recompressed @ 40MHz

nd Stage Fiber Amplifier pedestal Core Er-Yb co-doped Core: 5µm, 0.1NA Cladding: 300 µm, 0.46NA Single transverse mode output: Cladding Fiber made under AFRL LADERA Program

Mode quality

Amplified 1558-nm Signal Amplified Signal (W) 30 0 10 Slope efficiency=40% Max Power: 6W Rep Rate: 40MHz Stretched Pulse Duration: 80-ps 1-µm ASE: 15W 0 0 0 40 60 80 Coupled Pump Power (W)

Spatial Chirp for Tilted Incidence L y c d=lsinθ y = d Δλ / d=lsinθ=δλsin θ /c x y = 0 dδ λ =Δ λ sinθ /c c: chirp rate y = - d Δλ /

Spatial Chirp for Tilted Incidence (con t) + = = Δ Δ + Δ Δ 0 0 0 0 exp ) ( w d y erf w w d y erf w dr w r I y I d y d y λ λ π π λ λ 1/e beam-width w Chirp rate: 7.5nm/cm Incident beam-radius: 1-mm M = w /w 0 Incident angle < 3 M < 1.11 1.0 1. 1.4 1.6 0 4 6 8 incident angle (degree) M

Stretched Pulse: 80-ps 80-ps

Recompressed Pulse Spectrum 1.5 1.00 a.u. 0.75 0.50 0.5 0 1550 1555 1560 1565 1570 Wavelength (nm)

Recompressed Pulse : 1.1-ps 1.5 measured autocorrelation 15W measured autocorrelation 10W BW calculated autocorrelation 1.0 a.u. 0.5 0-5.0 -.5 0.5 5.0 pulse width (ps)

Self-Phase Modulation Distortion SPM induces a phase shift, which is equivalent to the action of a dispersive device with corresponding dispersion order * β SPM n = Pγz 0 eff d n ~ ( U o ~ U nom n dω ( ω) ) ω = 0 pulse shape distortion β 4 ~ 0.(ps 4 ) Φ peak =0.3=P 0 γz eff *Ultrashort-Pulsed Fiber Amplifier in Ultrafast Lasers: Technology and Applications, M. E. Fermann, A. Galvanauskas and G. Sucha, eds,.

CVBG Energy Scalability Photo-Thermo-Refractive (PTR) glass damage threshold >10-J/cm for ~1-ns pulses Volume grating clear aperture 5mmx5mm 1-J damage threshold for ~1-ns pulses (4mm beam diameter) Multi-mJ damage threshold for sub-picosecond pulses Recently demonstrated 00-µJ 1-ps recompressed pulsed using CVBG at 1064-nm

PM Version of Er/Yb Fiber Amplifier pedestal Core Er-Yb co-doped Core: 5µm, 0.1NA Cladding: 300 µm, 0.46NA Single transverse mode output: Fiber made under AFRL LADERA Program

Power characteristics amplified signal (W) 1 8 4 5-m long amplifier fiber Seed: 75-mW 1549-nm signal 35% slope efficiency Polarisation extinction ratio: 13-16dB 0 0 10 0 30 40 coupled pump power(w)

Summary 5-um Er/Yb LMA (non-pm and PM versions) High power compact fiber CPA using novel CVBG stretchers and compressors 15-W average power (recompressed), 1.1-ps pulsed fiber CPA system