LIGO-G050360-00-R LIGO R&D1 Possible consequences of high optical power on AdL optical coatings Dave Reitze UF.

Slides:



Advertisements
Similar presentations
Advanced LIGO1 Laser Induced Damage due to Particulate Contamination Billingsley, Gushwa, Phelps, Torrie, Zhang LVC meeting March 2014.
Advertisements

Ultrafast Experiments Hao Hu The University of Tennessee Department of Physics and Astronomy, Knoxville Course: Advanced Solid State Physics II (Spring.
Dr. Mike Nofziger 2010 “LASERS” Light Amplification by the Stimulated Emission of Radiation.
R.6.2 Lasery Optoelektronika 2014 Dr hab. inż. B. B. Kosmowski 1.
AMCF Materials Characterization School 2012 X-Ray Photoelectron Spectroscopy Tim Morgan.
May Chuck DiMarzio, Northeastern University ECE-1466 Modern Optics Course Notes Part 9 Prof. Charles A. DiMarzio Northeastern University.
22. Ultrashort x-ray pulses: High-Harmonic Generation
G v1Squeezed Light Interferometry1 Squeezed Light Techniques for Gravitational Wave Detection July 6, 2012 Daniel Sigg LIGO Hanford Observatory.
Lecture 10. AFM.
CNMFrascati 12/01/061 High Power Laser System for Advanced Virgo C.N.Man Design goals Present technology Other activities in the world Virgo+ and Laser.
Adaptive Optics for Wavefront Correction of High Average Power Lasers Justin Mansell, Supriyo Sinha, Todd Rutherford, Eric Gustafson, Martin Fejer and.
Short pulses in optical microscopy Ivan Scheblykin, Chemical Physics, LU Outline: Introduction to traditional optical microscopy based on single photon.
Dye lasers The gain medium in a dye lasers is a solution made with an organic dye molecule. The solution is intensely coloured owing to the very strong.
Progress on Laser Induced Damage Studies of Grazing Incidence Metal Mirrors Mark S. Tillack T. K. Mau Mofreh Zaghloul Laser-IFE Program Workshop May 31-June.
UV laser-induced damage to grazing- incidence metal mirrors M. S. Tillack, J. Pulsifer, K. Sequoia 4th US-Japan Workshop on Laser-Driven Inertial Fusion.
Chapter 5: Wave Optics How to explain the effects due to interference, diffraction, and polarization of light? How do lasers work?
Leslie St., Unit 11, Richmond Hill, ON L4B 3L8 Canada Phone Fax Single mode fibre transmission.
Status of the advanced LIGO laser O. Puncken, L. Winkelmann, C. Veltkamp, B. Schulz, S. Wagner, P. Weßels, M. Frede, D. Kracht.
Test mass dynamics with optical springs proposed experiments at Gingin Chunnong Zhao (University of Western Australia) Thanks to ACIGA members Stefan Danilishin.
October 30th, 2007High Average Power Laser Program Workshop 1 Long lifetime optical coatings for 248 nm: development and testing Presented by: Tom Lehecka.
1 The Status of Melody: An Interferometer Simulation Program Amber Bullington Stanford University Optics Working Group March 17, 2004 G D.
ULTRA-BROAD BANDWIDTH CAVITY ENHANCED ABSORPTION SPECTROSCOPY Paul S. Johnston Kevin K. Lehmann Department of Chemistry University of Virginia.
Anti-Reflection Coated Silica Windows for Electra Stuart Searles, John Sethian Naval Research Laboratory Washington, D.C. Russell Smilgys Science Applications.
Scanning Electron Microscope (SEM)
Tunable Mid-IR Frequency Comb for Molecular Spectroscopy
Thermal Compensation: The GEO and LIGO experience and requirements for advanced detectors Gregory Harry LIGO/MIT On behalf of the LIGO Science Collaboration.
Investigate Laser induced desorption (LID) of hydrogen retained in co-deposited layers on JT-60 open-divertor tile 20 ps-pulsed Nd:YAG laser for wide laser-intensity.
Thermal noise from optical coatings Gregory Harry Massachusetts Institute of Technology - on behalf of the LIGO Science Collaboration - 25 July
Absorption in bulk crystalline silicon and in the crystal surfaces Aleksandr Khalaidovski 1 Alexander Khalaidovski 1, Jessica Steinlechner 2, Roman Schnabel.
FEMTOSECOND LASER FABRICATION OF MICRO/NANO-STRUCTURES FOR CHEMICAL SENSING AND DETECTION Student: Yukun Han MAE Department Faculty Advisors: Dr. Hai-Lung.
1 Large Aperture Dielectric Gratings for High Power LIGO Interferometry LSC/Virgo Meeting, Baton Rouge March 19-22, 2007 Optics Working Group Jerald A.
Alvaro Sanchez Gonzalez Prof. Jon Marangos Prof. Jim Clarke
Gravitational Wave Detection Using Precision Interferometry Gregory Harry Massachusetts Institute of Technology - On Behalf of the LIGO Science Collaboration.
Absorption in bulk crystalline silicon and in the crystal surfaces Aleksandr Khalaidovski 1 Alexander Khalaidovski 1, Jessica Steinlechner 2, Roman Schnabel.
The investigation of optical inhomogeneities of the multilayer mirrors progress report Moscow State University Bilenko I.A
G Z LIGO R&D1 Input Optics Definition, Function The input optics (IO) conditions light from the pre- stabilized laser (PSL) for injection into.
DFG-NSF Astrophysics Workshop Jun 2007 G Z 1 Optics for Interferometers for Ground-based Detectors David Reitze Physics Department University.
Parametric Instabilities and Control Li Ju ( 鞠莉), Chunnnong Zhao, David Blair Jiayi Qin, Qi Fang, Carl Blair, Jian Liu University of Western Australia.
Industrial Affiliates Workshop, Feb Femtosecond enhancement cavities for generation of light at extreme wavelengths R. Jason Jones College of Optical.
LIGO-G ITM07 Postmortem H. Armandula, G. Billingsley, D.Cook, R. DeSalvo, G.Harry, B. Kells and L. Zhang LSC Meeting - March 2006.
V. Sonnenschein, I. D. Moore, M. Reponen, S. Rothe, K.Wendt.
LIGO-G M LIGO R&D1 Initial LIGO upgrade to 30 W: Implication for the Input Optics UFLIGO Group.
Thermoelastic dissipation in inhomogeneous media: loss measurements and thermal noise in coated test masses Sheila Rowan, Marty Fejer and LSC Coating collaboration.
Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group.
Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
Status of Modeling of Damage Effects on Final Optics Mirror Performance T.K. Mau, M.S. Tillack Center for Energy Research Fusion Energy Division University.
ACIGA High Optical Power Test Facility
Equivalence relation between non spherical optical cavities and application to advanced G.W. interferometers. Juri Agresti and Erika D’Ambrosio Aims of.
LIGO PAC Meeting, LIGO Hanford Observatory, November 29, 2001 LIGO-G Z Development of New Diagnostic Techniques for Preliminary and in Situ Characterization.
Heinert et al Properties of candidate materials for cryogenic mirrors 1 Properties of candidate materials for cryogenic mirrors D. Heinert,
G D Workshop on Optical Coating, March 20-21, The Coating Scattering and Absorption Measurements of LIGO I mirrors at Caltech Liyuan Zhang,
Chapter 9 Threshold Requirements. Looking at Loss again Laser medium R1R1 R2R2 d Loss/length =  1 Gain/length =  −  or  I I e -(  1+  d IR.
LIGO Scientific Collaboration
Optical Coatings for Gravitational Wave Detection Gregory Harry Massachusetts Institute of Technology - On Behalf of the LIGO Science Collaboration - August.
The coating thermal noise R&D for the 3rd generation: a multitechnique investigation E. Cesarini 1,2), M.Prato 3), M. Lorenzini 2) 1)Università di Urbino.
An H- stripping laser using commercial, diode-pumped Nd:YAG amplifiers Russell Wilcox Laser Stripping Workshop, April 11, 2011.
“LASERS” Light Amplification by the Stimulated Emission of Radiation.
LIGO-G D Core Optics Components (COC) Polishing Pathfinder Kickoff Advanced LIGO Project GariLynn Billingsley Caltech.
Surface-Enhanced Raman Scattering (SERS)
LIGO-G Z Bilenko I.A. Gromova E.S. 1 Recent Results on the Measurement of Transmission and Scattering Structure on Doped and Non-doped Mirrors.
Light-Matter Interaction
W. Kells LIGO Laboratory, Caltech C. Vorvick LIGO Laboratory, Hanford
Mark S. Tillack T. K. Mau Mofreh Zaghloul
ECEN 2010 April 28,2014 Frank Barnes.
LIGO Scientific Collaboration
Principle of Mode Locking
W. Kells LIGO Laboratory, Caltech C. Vorvick LIGO Laboratory, Hanford
AMO Early Science Capability
ITM03; LHO ITMx Post O2 inspection LIGO-T v1
OBSERVATION OF LEVEL-SPECIFIC PREDISSOCIATION RATES IN S1 ACETYLENE
Presentation transcript:

LIGO-G R LIGO R&D1 Possible consequences of high optical power on AdL optical coatings Dave Reitze UF

LIGO-G R LIGO R&D2 Some numbers Advanced LIGO Arm Cavities Design stored power is 800 kW »this is a lot of power »Compare LIGO 1 design: 18 kW For a 6 cm radius spot, intensity at mirror surface is 7 kW/cm 2 »Defined by 1/e criterion »Compare LIGO 1 design: 0.5 kW/cm 2 »This is actually not a very high intensity but it will be sustained over very long periods Advanced LIGO Mode Cleaner Design stored power is 100 kW »Compare LIGO 1: 3.4 kW For a 2.1 mm radius spot, intensity (flat mirror surfaces) is 720 kW/cm 2 »Higher intensity ! »Compare LIGO 1: 42 kW/cm 2

LIGO-G R LIGO R&D3 Summary of Ignorance Advanced LIGO is in a new regime »Very high average power and continuous wave operation »Military work in this area, but hard to get information Numerous investigations of damage thresholds by pulsed Nd:YAG lasers (NIF, Nova, ….), but few studies of CW damage »Damage mechanisms are different in pulsed and CW regimes »Most information comes from vendor studies »Typical reported CW damage threshold for Nd:YAG, 1064 nm is 1 MW/cm 2 –REO claims their coatings will handle higher intensities Some investigations of mirror contamination and damage for high average power synchrotron and FEL operation »High vacuum, but EUV (even X-ray) operation and pulsed »LLNL AVLIS program did some work on CW damage in the early 90’s

LIGO-G R LIGO R&D4 Issues we would like to understand better Damage thresholds, mechanisms »Powers and intensities are below typically quoted damage thresholds for CW laser damage, typically > 1 MW/cm 2 –Caveat #1: long term effects? –Caveat #2: Contamination-assisted? Surface nonlinear processes »Multi-photon surface bond-breaking –Hydrocarbon contamination –A nonlinear process, yet over years could be a problem Contamination »Solid evidence for surface contamination in LIGO based on LHO, LLO experiences –19 ppm HR surface absorption measured on H1 ITM –  15.2 W of absorbed power when extrapolated to AdL Weird stuff »Cosmic rays interacting with surface coatings? »Charging of coated surface  hydrocarbon sticking  surface photochemistry? »???

LIGO-G R LIGO R&D5 Recommendations I Talk to outside experts and collect information »CW mirror characteristics under high power: Northrup Grumman, TRW, LLNL »Contamination: we may be the experts in this field, but should talk to people at BNL, ALS, APS, JLAB, Stanford Experiment #1: Characterize damage thresholds of AdL optical coatings »Raster scan, 1 and 100 s exposures, fixed spot size, increasing power »Post-mortem microscopic examination –Well-established methods for quantitatively determining threshold Experiment #2: Assessment of long term effects of AdL intensities over sustained periods (~year) on mirror coatings »10 W into a F=20000 cavity with 1 mm spots  64 kW, 2 MW/cm 2 »10 -8 torr vacuum »Monitor: –Linewidth vs. time in situ –Surface second harmonic generation (look for green light from the surface) –Surface contamination vs time in situ Spatially-resolved sum frequency generation –Periodic surface inspections outside vacuum

LIGO-G R LIGO R&D6 Recommendations II LIGO 1 mode cleaner could provide some information relevant to AdL arm cavities »Worth doing a careful investigation of cavity properties now that 5 W is going into MC –Monitor linewidth periodically and consistently –Monitor MC REFL spot shape over time Comparison with MELODY »Next vacuum incursion into L1,H1,H2, visually inspect mirrors for problems Investigate possibilities for cleaning mirrors ? »“Reversible laser damage of dichroic coatings in a high average power laser vacuum resonator” by Chow, et al. –Near IR (55 kW/cm 2 ) and multi-line argon (1 kW/cm 2 ) irradiation –Degraded performance attributed to loss of surface O atoms Possible mechanisms for O depletion proposed »All attributed to Ar (green) irradiation –Irradiating degraded mirrors with 10 kW/cm 2 in 1-10 T O 2 restores performance by replacing O.

LIGO-G R LIGO R&D7 Damage threshold measurement Lens Shutter Mirror Nd:YAG ND filter Raster Scan post mortem analysis using optical microscopy, Nomarksi contrast microscope to identify threshold statistics required (100 shots) per fluence Graphic: Spica Optics

LIGO-G R LIGO R&D8 Surface Sum Frequency Generation k 3 R,  3 =  1 +  2 d Z k 1,  1 (near IR) k 2,  2 (tunable mid-IR) k 3 T,  3 =  1 +  2  m,  (2) m n 1 =  1 1/2 n 2 =  2 1/2 RR CH stretch of methanol at methanol vapour/liquid interface 1 = 532 nm, 2 = IR Resonant enhancement of SFG from chemical bonds of molecules present on surfaces Surface sensitive –  (2) contributes only at surface Non-contact, in situ High spatial resolution

LIGO-G R LIGO R&D9 Surface Contamination Monitoring Ultrafast Chirped Pulse Amplifier Optical Parametric Amplifier IR MIR IR Delay-line Vacuum Chamber Spectrometer IR + MIR 10 W Nd:YAG Laser