UCRL-POST-213237 High Average Power Frequency Conversion on the Laser Zhi M. Liao, Christopher Ebbers, Andy Bayramian, Mike Benapfl, Barry Freitas, Bob Kent, Dave van Lue, Kathleen Schaffers, Steve Telford, Peter Thelin, Everett Utterback, Camille Bibeau 1 National Ignition Facility Directorate Lawrence Livermore National Laboratory Livermore, California 94550 Bruce Chai, Yiting Fei Crystal Photonics, Inc. Sanford, Florida 32773 This work was performed under the auspices of the U. S. Department of Energy by the University of California, Lawrence Livermore National Laboratory under Contract No. W-7405-Eng-48.
Introduction The laser requires high efficiency frequency conversion at high average power. 1w Output 2w Output λ 1 λ 1 λ 2 TYPE I NLO Crystal Energy Pulse Width Drive PRF Avg. Power 100 J 3 ns 1 GW/cm 2 10 Hz 1000 W > 70 J > 700W Wavelength 1047 nm 523.5 nm We have investigated sapphire face cooling as well as helium gas cooling for active cooling of the nonlinear optical crystals. Bulk sapphire cooling Temperature gradients affect the refractive index (thermal dispersion) leading to phase mismatch across the crystal i.e. reduced conversion efficiency! Temperature gradients can also lead to internal stress and potential fracture!
Material Strategy We have examined the use of four commercially available nonlinear optical crystals with potential for scaling to large apertures Type I d eff (pm/v) Clear Aperture (dia. cm) Angular Acceptance (mrad-cm) Wavelength Acceptance (nm-cm) Absorption at 1 mm ( %/cm) Temperature Acceptance ( o C-cm) KDP 0.26 50+ 1.25 19.7 5 11 DKDP 0.23 50+ 1.34 5.2 0.1 11 YCOB 1.1 8.5 1.38 1.3 0.1 40 BBO 2.01 2 0.6 2.2 0.1 40 Large temperature acceptance makes BBO an ideal candidate but large aperture crystal growth is difficult. Large aperture high damage threshold DKDP is currently available. Thermal management is incorporated by utilizing multiple plates to obtain high conversion efficiency. YCOB offers the best thermal acceptance as well as high relative surface hardness. However, it is a relatively new crystal and requires development to obtain large aperture plates. Strategy - A two tiered approach DKDP: Low risk in acquiring large aperture parts. YCOB: A moderate risk R&D growth effort with potentially high performance.
DKDP Material O K O H KH 2 PO 4 is a hydrogen bonded water solution grown crystal Growth of KDP in heavy water (D 2 O) substitutes the heavier deuteron for hydrogen Optical absorption is shifted further to the infrared 5 Optical Absorption (%/cm) 4 3 2 1 0 0 20 40 60 80 100 Deuteration Level (%) The optical absorption in the near infrared is dramatically reduced with increasing deuteration level DKDP is harder to grow than KDP but 80% DKDP has been grown to 40 cm apertures
DKDP Frequency Converter The lower fracture toughness of the DKDP crystal implies that thinner slabs are required. Total Plates Total thickness FWHM Temperature 4 45 mm 2 C Four DKDP plate configuration DKDP utilizes sol-gel coatings for antireflection. A dual layer sol-gel AR coating is applied to both surfaces (for both 1047 and 523.5 nm). %Reflectance@2w Mean = 0.51148 Min = 0.097900 Max = 3.4777 Std Dev = 0.47661 Uniformity = 93.183 % 3.48 2.91 2.35 1.79 1.22 0.66 0.10 Slab#1 Slab#2 Slab#3 Slab#4 Single DKDP test plate configuration Mean Reflectivity @ 1ω [%] Mean Reflectivity @ 2ω [%] 0.73 0.51 0.69 0.57 0.71 0.52 0.64 0.56
DKDP Experiment We utilized CaF 2 (awaiting sapphire delivery) to test the heat spreader concept. The heat spreader technology was demonstrated with a single plate of DKDP and CaF 2 (a substitute for sapphire) at repetition rate (3.3 Hz). DKDP Tuning Data DKDP Tuning 100 Frequency Conversion @ 3.3 Hz 1.0 Norm. Conv. Efficiency 0.8 0.6 0.4 0.2 0.0-2.5-2 -1.5-1 -0.5 0 0.5 1 1.5 2 2.5 Energy (J) 10 1ω 2ω 1w 2w Angle (urad) Internal angular acceptance is measured to be 1.3 mrad-cm (consistent with calculations). 1 0 2 4 6 8 Shots (x10 3 ) No damage to the DKDP-CaF 2 cooler interface was observed up to the 55 J energy level. The 2w power decrease observed in the DKDP during 3.3 Hz operation is consistent with calculations using CaF 2 instead of sapphire.
YCOB Material Tremendous progress has been made on growing large size, optical quality YCOB boules. Previous efforts 1999 1/2005 YCOB advantages 3x thermal conductivity of KDP and DKDP 3x nonlinear coefficient of DKDP (thinner crystal) Equivalent 3ω bandwidth of DKDP Thermally insensitive operation at 2ω Hardness of quartz takes hard AR coating 2000 9/2004 frequency converter size LLNL and CPI efforts
YCOB Frequency Converter Full Size YCOB slabs will utilize face-cooling technology with bulk sapphire plates. Edge-cooled single plate of YCOB 1ω near field 2ω near field YCOB First Green Light! YCOB Tuning Data YCOB Tuning Norm. Efficiency 1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0-4 -3-2 -1 0 1 2 3 4 angle (urad) Internal angular acceptance is measured to be 1.2 mrad-cm (consistent with calculations).
YCOB Experiment A single plate of edge-cooled YCOB was demonstrated at high average power (0.55 kw input) and high repetition rate (10 Hz). 1w Output Energy (J) 100 90 80 70 60 50 40 30 20 10 1w 2w Energy Data 1w Output 2w 0 0 5 10 15 20 25 30 Number of Shots (x 10 3 ) Normalized Intensity 1.0 0.8 0.6 0.4 0.2 0.0 2w 1w 0 5 10 15 20 25 30 Time (ns) Conversion Efficiency (%) 80 70 60 50 40 30 20 10 Conversion Efficiency 0 0.00 0.02 0.04 0.06 0.08 0.10 0.12 0.14 0.16 1w Intensity (GW/cm2) We successfully operated the YCOB frequency converter up to 0.5 kw of 1w drive with 50% conversion efficiency. Higher efficiency is expected at higher drives.
Summary The laser requires high efficiency frequency conversion at high average power. We have implemented a two-tier frequency conversion risk-reduction plan that employs the use of DKDP and YCOB for the frequency conversion crystal. We have successfully demonstrated a single plate face cooled DKDP SHG module. We have obtained full-size apertures crystals of YCOB. We have successfully operated a YCOB frequency converter at high average power (15 ns, 10 Hz, 227W @ 523.5 nm) with a conversion efficiency of 50%. Higher efficiency is expected with shorter pulse widths and improved beam quality.