Self-optimizing additive pulse mode-locked fiber laser: wavelength tuning and selective operation in continuous-wave or mode-locked regime

Similar documents
Testing with Femtosecond Pulses

Elimination of Self-Pulsations in Dual-Clad, Ytterbium-Doped Fiber Lasers

Mechanism of intrinsic wavelength tuning and sideband asymmetry in a passively mode-locked soliton fiber ring laser

R. J. Jones College of Optical Sciences OPTI 511L Fall 2017

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

Timing Noise Measurement of High-Repetition-Rate Optical Pulses

How to build an Er:fiber femtosecond laser

taccor Optional features Overview Turn-key GHz femtosecond laser

Designing for Femtosecond Pulses

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband

Directly Chirped Laser Source for Chirped Pulse Amplification

The Theta Laser A Low Noise Chirped Pulse Laser. Dimitrios Mandridis

A new picosecond Laser pulse generation method.

Picosecond Pulses for Test & Measurement

Cost-effective wavelength-tunable fiber laser using self-seeding Fabry-Perot laser diode

Recent Progress in Pulsed Optical Synchronization Systems

Wavelength switching using multicavity semiconductor laser diodes

Extending the Offset Frequency Range of the D2-135 Offset Phase Lock Servo by Indirect Locking

TIGER Femtosecond and Picosecond Ti:Sapphire Lasers. Customized systems with SESAM technology*

Yb-doped Mode-locked fiber laser based on NLPR Yan YOU

First published on: 22 February 2011 PLEASE SCROLL DOWN FOR ARTICLE

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

Optical generation of frequency stable mm-wave radiation using diode laser pumped Nd:YAG lasers

All-fiber, all-normal dispersion ytterbium ring oscillator

Testing with 40 GHz Laser Sources

Introduction Fundamental of optical amplifiers Types of optical amplifiers

SUPPLEMENTARY INFORMATION

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

Applied Physics Springer-Verlag 1981

Quantum-Well Semiconductor Saturable Absorber Mirror

Fast Widely-Tunable CW Single Frequency 2-micron Laser

A continuous-wave Raman silicon laser

Active mode-locking of miniature fiber Fabry-Perot laser (FFPL) in a ring cavity

SUPPLEMENTARY INFORMATION DOI: /NPHOTON

A 40 GHz, 770 fs regeneratively mode-locked erbium fiber laser operating

Stable dual-wavelength oscillation of an erbium-doped fiber ring laser at room temperature

Generation of gigantic nanosecond pulses through Raman-Brillouin- Rayleigh cooperative process in single-mode optical fiber

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

Optical phase-coherent link between an optical atomic clock. and 1550 nm mode-locked lasers

Fast Raman Spectral Imaging Using Chirped Femtosecond Lasers

High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W

Spectral Phase Modulation and chirped pulse amplification in High Gain Harmonic Generation

Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism

Solid-State Laser Engineering

Generation and evolution of mode-locked noiselike square-wave pulses in a large-anomalousdispersion Er-doped ring fiber laser

Tunable erbium ytterbium fiber sliding-frequency soliton laser

25 W CW Raman-fiber-amplifier-based 589 nm source for laser guide star

Study of Multiwavelength Fiber Laser in a Highly Nonlinear Fiber

Improvement of terahertz imaging with a dynamic subtraction technique

PITZ Laser Systems. Light Amplification by Stimulated Emission of Radiation. Cavity. What is a Laser? General introduction: systems, layouts

Fundamental Optics ULTRAFAST THEORY ( ) = ( ) ( q) FUNDAMENTAL OPTICS. q q = ( A150 Ultrafast Theory

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

1550 nm Programmable Picosecond Laser, PM

Wavelength-independent coupler from fiber to an on-chip cavity, demonstrated over an 850nm span. Steven Wang, Tal Carmon, Eric Ostby and Kerry Vahala

THE TUNABLE LASER LIGHT SOURCE C-WAVE. HÜBNER Photonics Coherence Matters.

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

Data sheet for TDS 10XX system THz Time Domain Spectrometer TDS 10XX

Analysis of Self-Pulsation in Distributed Bragg Reflector Laser based on Four-Wave Mixing

UNMATCHED OUTPUT POWER AND TUNING RANGE

Pulse breaking recovery in fiber lasers

Highly Reliable 40-mW 25-GHz 20-ch Thermally Tunable DFB Laser Module, Integrated with Wavelength Monitor

RF-Based Detector for Measuring Fiber Length Changes with Sub-5 Femtosecond Long-Term Stability.

771 Series LASER SPECTRUM ANALYZER. The Power of Precision in Spectral Analysis. It's Our Business to be Exact! bristol-inst.com

Fiber-based components. by: Khanh Kieu

ModBox-OBand-56GBaud-PAM4 O-Band, 56 Gbaud PAM-4 Reference Transmitter

Lab 5 - Electro-Optic Modulation

Optical spectra beyond the amplifier bandwidth limitation in dispersion-managed mode-locked fiber lasers

R. J. Jones Optical Sciences OPTI 511L Fall 2017

Narrowband PMD Measurements with the Agilent 8509C Product Note

Single-Walled Carbon Nanotubes for High-Energy Optical Pulse Formation

Fiber Laser Chirped Pulse Amplifier

Laser Transmitter Adaptive Feedforward Linearization System for Radio over Fiber Applications

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

DISPERSION MEASUREMENT FOR ON-CHIP MICRORESONATOR. A Thesis. Submitted to the Faculty. Purdue University. Steven Chen. In Partial Fulfillment of the

All optical wavelength converter based on fiber cross-phase modulation and fiber Bragg grating

Mitigation of Self-Pulsing in High Power Pulsed Fiber Lasers

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

A transportable optical frequency comb based on a mode-locked fibre laser

Swept Wavelength Testing:

quantiflash Calibration Light Source for Cytometry

Wavelength Control and Locking with Sub-MHz Precision

A NOVEL SCHEME FOR OPTICAL MILLIMETER WAVE GENERATION USING MZM

High-Power Femtosecond Lasers

It s Our Business to be EXACT

All-Optical Signal Processing and Optical Regeneration

Setup of the four-wavelength Doppler lidar system with feedback controlled pulse shaping

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression

NOW WITH BROADER TUNING RANGE

Electro-optic Spectral Decoding Measurements at FLASH

Drive Laser State-of-the-art: Performance, Stability and Programmable Repetition Rate The Jefferson Lab Experience

SCTE. San Diego Chapter March 19, 2014

Demonstration of directly modulated silicon Raman laser

9) Describe the down select process that led to the laser selection in more detail

DBR based passively mode-locked 1.5m semiconductor laser with 9 nm tuning range Moskalenko, V.; Williams, K.A.; Bente, E.A.J.M.

pulsecheck The Modular Autocorrelator

HIGH-PRECISION LASER MASTER OSCILLATORS FOR OPTICAL TIMING DISTRIBUTION SYSTEMS IN FUTURE LIGHT SOURCES

Mode-Locked Diode Laser for Precision Optical Frequency Measurements

ModBox-850nm-NRZ-series

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

Transcription:

Self-optimizing additive pulse mode-locked fiber laser: wavelength tuning and selective operation in continuous-wave or mode-locked regime Manuel Ryser, Christoph Bacher, Christoph Lätt, Alexander Heidt, Philippe Raisin, Thomas Feurer, Valerio Romano Institute of Applied Physics, University of Bern, Switzerland January 31, 2018 Paper No. 10512-47 Conference 10512: Fiber Lasers XV: Technology and Systems Session: Mode-locked Fiber Oscillators

Motivation and Vision From todays femtosecond fiber-laser systems... mode-locking regime often lost due to temperature drift or mechanical disturbance no tuning or critical parameters possible long term stable operation only in lab-like conditions...towards self-optimizing fiber laser systems. online-monitoring (optical spectrum, RF spectrum etc.) electronic tuning of fiber-optic components (filters, couplers, polarization controllers) global opimization algorithms for efficient self-optimization continuous supervision and fine adjustments

All-normal Dispersion Fiber Ring Laser total cavity fiber length approx. 39.5 m CONS not long term stable alignment of three waveplates not trivial PRO operational parameter can be varied experimentally

high-resolution mapping procedure servo: 180 travel range, 8bit resolution 180 /256 steps = 0.7 stepsize; 256^3 = 16'777'216 servo positions 180 /64 steps = 2.8 stepsize; 64^3 = 262'144 servo positions

Data Evaluation detector [V] 1.2 1.0 0.8 0.6 0.4 0.2 oscilloscope trace optical spectrum radio-frequency spectrum 0.0 0.5 1.0 time [µs] number of pulses in cavity: harmonic mode-locking? T 1.5 intensity [db] -20-30 -40-50 -60 1000 1020 FWHM FW20dB λ max λ c 1040 1060 wavelength [nm] 0dB -3dB -20dB 1080 1100 by inverse fourier transform estimate of transform limited pulse duration ττ pppppppppp amplitude [dbm] -20-40 -60-80 0 P A 20 pulse energy jitter f 1 f 2 f 3 f 4 f 5 P B 40 1/T 60 80 RF frequency [MHz] EE EE P C 100 PP CC PP AA 1 temporal pulse jitter tt TT PP BB PPAA nn nn D. Von der Linde, Appl. Phys. B 39, 201-217 (1986)

Data Evaluation detector [V] 1.2 1.0 0.8 0.6 0.4 0.2 oscilloscope trace optical spectrum radio-frequency spectrum 0.0 T 0.5 1.0 time [µs] 1.5 intensity [db] -20-30 -40-50 -60 1000 1020 FWHM FW20dB λ max λ c 1040 1060 wavelength [nm] 0dB -3dB -20dB 1080 1100 amplitude [dbm] -20-40 -60-80 0 P A f 1 f 2 f 3 f 4 f 5 P B 20 40 1/T 60 80 RF frequency [MHz] P C 100 detector [V] 1.0 0.8 0.6 0.4 0.2 0.0 0.5 T 1.0 time [µs] 1.5 intensity [db] 2.0-20 -30-40 -50 1020 FWHM FW20dB λ c λ max 1030 1040 wavelength [nm] 0dB -3dB -20dB 1050 amplitude [dbm] -20-40 -60-80 0 P A 1/T f 1 f 2 f 3 f 4 f 5 P C 20 40 60 80 100 RF frequency [MHz]

High-resolution maps map of wavelength λλ cc tunable briefringent filter [1] map of pulse energy jitter log EE EE log PP CC PP AA 1 tunable saturable absorber [2] [1] Humphrey, P. and Bowers, J. (1993). [2] Haus, H., Ippen, E., and Tamura, K. (1994).

Histogram of pulse energy jitter - operation modes double line CW 13.5 THz 1.4 THz mode-locked RAMAN single line CW

map of mode-locked operation mode EE EE < 0.01 color coded with wavelength clusters with mode-locked areas at different wavelengths each cluster covers approx. 20 nm wavelength tunable with waveplates overall tunability approx. 55 nm

map of continuous-wave operation mode EE EE = 0.1 0.11 color coded with wavelength band-like structure each band covers approx. 20 nm wavelength tunable with waveplates overall tunability approx. 55 nm

Self-optimization with genetic algorithm

Single objective genetic algorithm objective: pulse energy jitter operation mode at "best" setting: optical spectrum RF spectrum population size of 50 individuals algorithm converges after approx. 35 generations 50*35 = 1'750 servo positions to be evaluated until convergence (16'777'216 servo positions for full 3D scan --> 0.01%)

Multi-objective genetic algorithm optical spectrum RF spectrum population size optical of 50 spectrum individuals optical spectrum algorithm converges after approx. 284 generations 50*284 = 14'200 servo positions to be evaluated until convergence (16'777'216 servo positions for full 3D scan --> 0.08%) RF spectrum RF spectrum

Summary & Outlook Experimental Setup: automated all-normal dispersion additive pulse mode-locked fiber laser High-resolution three dimensional maps: pulse-energy jitter: allows to discriminate between different operating regimes lasing wavelength: tunable over more than 55nm for CW and mode-locked operation Self-optimization by genetic-algorithm towards desired operating state: single-objective: mode-locked multi-objective: mode-locked at desired wavelength Outlook map of further parameters: pulse duration, timing jitter, harmonic mode-locking include these parameters into multi-objective optimization by genetic algorithm include pump power into optimization