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

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

Review of MPS Solid State Laser Systems

Power Scaling of Tm:fiber Lasers to the kw Level

High-power, high-energy diode-pumped Tm:YLF-Ho:YLF laser

High-power operation of Tm:YLF, Ho:YLF and Er:YLF lasers

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

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

High-Power Femtosecond Lasers

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

Directly Chirped Laser Source for Chirped Pulse Amplification

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

High Power and Energy Femtosecond Lasers

Femtosecond pulse generation

taccor Optional features Overview Turn-key GHz femtosecond laser

Designing for Femtosecond Pulses

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

Survey Report: Laser R&D

Development of Nano Second Pulsed Lasers Using Polarization Maintaining Fibers

Continuum White Light Generation. WhiteLase: High Power Ultrabroadband

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

Romania and High Power Lasers Towards Extreme Light Infrastructure in Romania

156 micro-j ultrafast Thulium-doped fiber laser

Survey Report: Laser R&D

Development of scalable laser technology for EUVL applications

VELA PHOTOINJECTOR LASER. E.W. Snedden, Lasers and Diagnostics Group

High Energy Non - Collinear OPA

Thin-Disc-Based Driver

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

Fiber lasers: The next generation

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

How to build an Er:fiber femtosecond laser

1550 nm Programmable Picosecond Laser, PM

Vertical External Cavity Surface Emitting Laser

pulsecheck The Modular Autocorrelator

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

Fiber Laser Chirped Pulse Amplifier

APE Autocorrelator Product Family

Spider Pulse Characterization

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

Fiber Lasers for EUV Lithography

Laser Development at Q-Peak for Remote Sensing. Peter Moulton Q-Peak, Inc. MRS Spring Meeting March 29, 2005 Paper FF1.1

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

High Average Power, High Repetition Rate Side-Pumped Nd:YVO 4 Slab Laser

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

Regenerative Amplification in Alexandrite of Pulses from Specialized Oscillators

FPPO 1000 Fiber Laser Pumped Optical Parametric Oscillator: FPPO 1000 Product Manual

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

dnx/dt = -9.3x10-6 / C dny/dt = -13.6x10-6 / C dnz/dt = ( λ)x10-6 / C

Ultrafast instrumentation (No Alignment!)

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

Ultrafast Laser Solutions for Microprocessing

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

Thesis. Submitted to. The School of Engineering of the UNIVERSITY OF DAYTON. In Partial Fulfillment of the Requirements for.

PGx11 series. Transform Limited Broadly Tunable Picosecond OPA APPLICATIONS. Available models

Ultrafast amplifiers

5kW DIODE-PUMPED TEST AMPLIFIER

Testing with Femtosecond Pulses

Theoretical Approach. Why do we need ultra short technology?? INTRODUCTION:

A new picosecond Laser pulse generation method.

Recent Progress on the 10PW laser Project at SIOM

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

Generation of 15-nJ pulses from a highly efficient, low-cost. multipass-cavity Cr 3+ :LiCAF laser

FA Noncollinear Optical Parametric Amplifier

Faraday Rotators and Isolators

Quantum-Well Semiconductor Saturable Absorber Mirror

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

6.1 Thired-order Effects and Stimulated Raman Scattering

Chirped Pulse Amplification

UNMATCHED OUTPUT POWER AND TUNING RANGE

Development of high average power fiber lasers for advanced accelerators

The Proposed MIT X-ray Laser Facility: Laser Seeding to Achieve the Transform Limit

Supplementary Information for

Laser systems for science instruments

A 243mJ, Eye-Safe, Injection-Seeded, KTA Ring- Cavity Optical Parametric Oscillator

Recent Progress in Pulsed Optical Synchronization Systems

Supplementary Materials for

Bioimaging of cells and tissues using accelerator-based sources

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

Mira OPO-X. Fully Automated IR/Visible OPO for femtosecond and picosecond Ti:Sapphire Lasers. Superior Reliability & Performance. Mira OPO-X Features:

Large-aperture chirped volume Bragg grating based fiber CPA system

Gigashot TM FT High Energy DPSS Laser

Multi-Wavelength, µm Tunable, Tandem OPO

Laser Science and Technology at LLE

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

Supercontinuum Sources

Nd: YAG Laser Energy Levels 4 level laser Optical transitions from Ground to many upper levels Strong absorber in the yellow range None radiative to

PERFORMANCE OF PHOTODIGM S DBR SEMICONDUCTOR LASERS FOR PICOSECOND AND NANOSECOND PULSING APPLICATIONS

Development of Mid-infrared Solid-State Lasers

SNP High Performances IR Microchip Series

Spectral phase shaping for high resolution CARS spectroscopy around 3000 cm 1

Single frequency MOPA system with near diffraction limited beam

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression

Ultrafast Lasers with Radial and Azimuthal Polarizations for Highefficiency. Applications

Improving efficiency of CO 2

A CW seeded femtosecond optical parametric amplifier

Laser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography

High-Conversion-Efficiency Optical Parametric Chirped-Pulse Amplification System Using Spatiotemporally Shaped Pump Pulses

SNP High Performances IR Microchip Series

Power. Warranty. 30 <1.5 <3% Near TEM ~4.0 one year. 50 <1.5 <5% Near TEM ~4.0 one year

THE ORION PHOTOINJECTOR: STATUS and RESULTS

Transcription:

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

Topics Diode-pumped Cr:ZnSe femtosecond oscillator CPA Cr:ZnSe laser system with 1 GW output This work was supported by SBIR Phase II programs from AFRL and DoE

Motivation Goals: Development of a low-noise, mode-locked femtosecond laser source at 2.5 m Development of high-energy, high-peak-power femtosecond laser source at 2.5 m Some applications: High-power amplifier seeding (for oscillator) Mid-IR super-continuum generation High-harmonic generation

Ti:Sapphire of infrared, courtesy Sorokin(a) Cr:ZnSe Ti:Sapphire Crystal structure Cubic Uniaxial Thermal conductivity 18 W/m C 28 W/m C Thermooptics dn/dt 70 10-6 1/ C 12 10-6 1/ C Third order nonlinearity n 2 180 10-20 m 2 /W at 1.6 µm*) 3 10-20 m 2 /W Two-photon absorption band gap 2.83 ev ~8 ev Second-order nonlinearity very high: 30 pm/v absent Peak emission cross-section em at 0 13 10-19 cm 2 2450 nm 4.5 10-19 cm 2 780 nm Fluorescence bandwidth 1000 nm (50 THz) 300 nm (130 THz) Relative bandwidth 0 0.49 0.57 Lifetime at room temp. 6 µs 3 µs E sat = h / em 0.06 J/cm 2 0.6 J/cm 2 I sat = h / em 11 kw/cm 2 210 kw/cm 2 Direct diode pumping Yes (cw) Emerging (cw)

Pumping options for Cr 2+ -doped lasers Er:fiber Tm:YALO Tm:YAG Tm:fiber Ho:YLF InGaAsP diodes Co:MgF 2 GaSb diodes Cr:ZnS Cr:ZnSe 1200 1400 1600 1800 2000 2200 2400 2600 Wavelength, nm

Diode-pumped Cr:ZnSe femtosecond oscillator SESAM M5 M4 M1 output 4 mm xtal 50 um spot 60% abs. sapphire M3 M2 Cr 2+ :ZnSe L4 L3 L2 L1 wavelength 1550 nm 3.5 W, diode laser M1-2% T output coupler; M2 ROC=100 mm; M3 ROC=150 mm; M4 flat HR; M5 ROC=100 mm; L1-4 collimating-focusing telescope.

Photograph of oscillator in enclosure

Characterization of the laser output autocorrelation intensity, a.u. 0.025 0.02 0.015 0.01 0.005 180 fs x 1.47 0-600 -400-200 0 time, fs 200 400 600 intensity, a.u. 1.7 1.6 1.5 1.4 1.3 2425 2475 2525 2575 wavelength, nm Autocorrelation trace of 180 fs pulse Spectrum of the laser output centered at 2520 nm with 30 nm bandwidth Pave = 50 mw

RF spectra of Cr:ZnSe femtosecond lasers Output of laser pumped by cw Er:fiber-pumped Tm:fiber laser Output of laser pumped by 1550-nm diode laser

Topics Diode-pumped Cr:ZnSe femtosecond oscillator CPA Cr:ZnSe laser system with 1 GW output This work was supported by SBIR Phase II programs from AFRL and DoE

Setup of typical CPA Ti:Sapphire system SHG CW Nd:doped pump laser 5 W at 532 nm SHG Nd:doped Q-switched pump laser 5 mj, 532 nm femtosecond KLM mode-locked Ti:S laser 10-50 fs, 10 nj, 800 nm 100 MHz Pulse stretcher Ti:S regenerative amplifier 1 mj, 800 nm output 800 nm, 30-100 fs, mj-j Pulse compressor Ti:S amplifier 800 nm SHG Nd:doped Q-switched pump laser

Fiber-laser-pumped Cr:ZnSe CPA system Tm:fiber 1940-nm polarized laser Tm:fiber 1940-nm laser 40 W 2050 nm Q-switched Ho:YLF laser 4.6 W 11 mj, 20 ns pulses 1 khz PRR Cr:ZnSe 2500 nm mode-locked laser 150 fs, 2.3 nj, 100 MHz CVBG Pulse stretcher 150 fs 300 ps Cr:ZnSe regenerative amplifier gain 6 x 10 5 0.7 mj pulses 1 khz PRR 2475 nm 0.35 mj pulses 346 fs Grating pulse compressor

Ho:YLF MOPA output Ho:YLF AMP DM HR Output power 11 W L1 DM L2 OC Ho:YLF OSC DM λ/2 Repetition rate 1 khz Pulse duration 20 ns 40 W Tm:fiber laser TFP DM HR AOM L3 12 10 HR output power, W 8 6 4 2 0 10 20 30 40 pump power, W

Regenerative amplifier Ho:YLF MOPA M1 λ = 2050 nm 11 W (1kHz) M3 L2 L1 M4 Cr 2+ :ZnSe M2 l/4 M6 RTP Regenerative amplifier TFP l/2 FR TFP Seed ~300 ps 1.2 nj M2 M5 Output 0.7 mj 1.5 cm single crystal 10 round trips

Stretcher-compressor pair ps out REGEN fs out seed M M AMP out TFP CVBG λ/2 M M G2 G1 M Stretcher CVBG 150 fs -> 300 ps Compressor (ruled diffraction gratings) 300 ps -> 350 fs

CPA system photograph

CPA output characterization 0.035 0.6375 autocorrelation intensity, a.u 0.03 0.025 0.02 0.015 0.01 experiment gaussian fit 346 fs X 1.47 intensity, a.u. 0.6325 0.6275 0.6225 0.005 0.6175 0-800 -600-400 -200 0 time, fs 200 400 600 800 0.6125 2400 2450 2500 2550 wavelength, nm Autocorrelation trace of 346 fs pulse Spectrum of the CPA output centered at 2475 nm with 30 nm bandwidth

> 1 kw of Tm:fiber power output at 2045 nm MOPA output power (W) 1200 1000 800 600 400 One stage Fiber #1 One stage Fiber #2 Two stage 61.6% slope efficiency 53.2% slope efficiency 200 0 0 200 400 600 800 1000 1200 1400 1600 1800 2000 Pump power (W)

2.05- m Ho:YLF MOPA scaling (Dergachev) Tm-pump #1 ~120 W at 1940 nm Osc/ Amp #1 Ho-stage/ Regime CW 100 Hz 500 Hz Tm-pump #2 ~120 W at 1940 nm Tm-pump #3 ~120 W at 1940 nm Amp #2 Amp #3 Osc/Amp #1 39 W 55 mj 50 mj Amp#2 76 W 110 mj 95 mj Amp#3 115 W 170 mj 140 mj Tm-fiber laser TLR-100-1940 IPG Photonics www.ipgphotonics.com Operation regime Beam Profile Output power Wavelength Polarization Linewidth CW TEMoo 120 W 1940 nm Random 2 nm

Summary We have developed a directly diode-pumped femtosecond Cr:ZnSe oscillator 180 fs pulsewidth We have built and operated the first Cr:ZnSe-based CPA system 1 GW peak power (350 fs, 0.35 mj) at a 1-kHz rate 2475 nm center wavelength Future: Improved SESAMs with broader spectral coverage Further CPA scaling with Q-switched Ho:YLF pumps