G060185-00-Z 1 eLIGO/advLIGO FI update Antonio Lucianetti, K.L. Dooley, R. Martin, L. F. Williams, M.A. Arain, V. Quetschke, G. Mueller, D.B. Tanner, and.

Slides:



Advertisements
Similar presentations
Optics, Eugene Hecht, Chpt. 8
Advertisements

Advanced LIGO1 Laser Induced Damage due to Particulate Contamination Billingsley, Gushwa, Phelps, Torrie, Zhang LVC meeting March 2014.
Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford.
Thermal Compensation System – TCS Technical Presentation aLIGO NSF Review LIGO Livingston Observatory April LIGO-G v5.
G R LIGO Laboratory1 Advanced LIGO Research and Development David Shoemaker LHO LSC 11 November 2003.
An Introduction to Omega and Omega EP Frequency Conversion Crystals.
High Power Input Optics for Advanced Virgo Julien Marque, Benjamin Canuel, Richard Day, Eric Génin, Flavio Nocera, Federico Paoletti The European Gravitational.
Currently: 3 year ( ) NSF-supported UF/IAP collaborative project "Methods and Instruments for High-Precision Characterization of LIGO Optical Components"
rd ILIAS-GW annual general meeting 1 VIRGO Commissioning progress J. Marque (EGO)
Particle flux simulations Sergei Striganov Fermilab June 11, 2008.
Laser Interferometer Gravitational-wave Observatory1 Characterization of LIGO Input Optics University of Florida Thomas Delker Guido Mueller Malik Rakhmanov.
G v1 Squeezer Update Review August 25, 2009 H1 Squeezer Experiment ANU, AEI, MIT, CIT and LHO collaboration.
Integration and Alignment of Optical Subsystem Roy W. Esplin Dave McLain.
G D Tasks After S3 Commissioning Meeting, Oct 6., 2003 Peter Fritschel, Daniel Sigg.
G D 1 Modulators and Isolators for Advanced LIGO 28 April 2006 UF LIGO group.
1 G Mike Smith Gravitational Waves & Precision Measurements.
Status of the advanced LIGO laser O. Puncken, L. Winkelmann, C. Veltkamp, B. Schulz, S. Wagner, P. Weßels, M. Frede, D. Kracht.
ILIAS WG1 meeting, 19/06/07 IB Faraday Isolator 1 IB in vacuum Faraday isolator E. Genin, S. Hebri, S. Hamdani, P. La Penna, J. Marque EGO.
LSC meeting, HLO, August 18, 2004 IAP/UF/LIGO Research Collaboration: Status and Prospectives Efim Khazanov, Ilya Kozhevatov, Anatoly Malshakov, Oleg Palashov,
aLIGO EOM at LLO and LHO Assembly/testing/installation
LIGO-G M May 31-June 2, 2006 Input Optics (IO) Cost and Schedule Breakout Presentation NSF Review of Advanced LIGO Project David Reitze UF.
LIGO-G Advanced LIGO Detector upgrade is planned for »Factor of 10 increase in distance probed (‘reach’) »Factor of 1000 increase in event.
LIGO-G D Enhanced LIGO Kate Dooley University of Florida On behalf of the LIGO Scientific Collaboration SESAPS Nov. 1, 2008.
Paolo La Penna The New Virgo Injection BenchN5-WP1 4 TH MEETING, Hannover, 7/04/2005 The New VIRGO Injection Bench Paolo La Penna European Gravitational.
European Gravitational Observatory12/12/2005 WG1 Hannover 1 Mode Matching of the Fabry-Perrot cavities Julien Marque.
Thermal Compensation in Stable Recycling Cavity 21/03/2006 LSC Meeting 2006 UF LIGO Group Muzammil A. Arain.
LIGO- G D The LIGO Instruments Stan Whitcomb NSB Meeting LIGO Livingston Observatory 4 February 2004.
1 Wan Wu, Volker Quetschke, Ira Thorpe, Rodrigo Delgadillo, Guido Mueller, David Reitze, and David Tanner Noise associated with the EOM in Advanced LIGO.
G Z LIGO R&D1 Input Optics Definition, Function The input optics (IO) conditions light from the pre- stabilized laser (PSL) for injection into.
50 W Laser Concepts for Initial LIGO Lutz Winkelmann, Maik Frede, Ralf Wilhelm, Dietmar Kracht Laser Zentrum Hannover LSC March 05 Livingston G Z.
DFG-NSF Astrophysics Workshop Jun 2007 G Z 1 Optics for Interferometers for Ground-based Detectors David Reitze Physics Department University.
Today’s topic Alignment Polarization Mechanism 1.
LSC August G Z Gingin High Optical Power Test Facility (AIGO) 1 High Optical Power Test Facility - Status First lock, auto-alignment and.
G TCS installation & results at LLO Update: Systems Telecon 8 th Jan 2014 Aidan Brooks (for the TCS Team) G v1.
Paolo La Penna Injection optics for Advanced VirgoLSC/VIRGO joint meeting, Cascina, 25/05/ Advanced VIRGO Input optics LIGO-G Z.
Split Electrode Wedged RTP crystal To avoid the unwanted generation of amplitude modulation by polarization modulation because of imperfect alignment of.
LIGO-G R High power optical components for Enhanced and Advanced LIGO Optics/Lasers WG, March 21, 2007 Volker Quetschke, Muzammil Arain, Rodica.
1/10 Tatsuya KUME Mechanical Engineering Center, High Energy Accelerator Research Organization (KEK) ATF2-IN2P3-KEK kick-off meeting (Oct. 10, 2006) Phase.
Engineering Division 1 M321/M331 Mirror Switchyard Design Review Tom Miller
LIGO-G0200XX-00-M LIGO Scientific Collaboration1 eLIGO Input Optics Characterization and Performance Kate Dooley University of Florida.
LIGO-G M LIGO R&D1 Initial LIGO upgrade to 30 W: Implication for the Input Optics UFLIGO Group.
Non-ideal Cavity Ring-Down Spectroscopy: Linear Birefringence, Linear Polarization Dependent Loss of Supermirrors, and Finite Extinction Ratio of Light.
G D LIGO Commissioning Update LSC Meeting, Nov. 11, 2003 Daniel Sigg.
New emittance monitor beamline
LIGO PAC Meeting, LIGO Hanford Observatory, November 29, 2001 LIGO-G Z Development of New Diagnostic Techniques for Preliminary and in Situ Characterization.
LIGO-G Z High Power Components for Advanced LIGO University of Florida Rupal Amin, Joe Gleason, Rachel Parks Christina Leidel, Mike Marquez, Luke.
Cascina, Nov. 4 th, 2008 AdV review 1 AdV Injection system E. Genin European Gravitational Observatory.
LIGO Scientific Collaboration Lasers and Optics Working Group 6 Month Report to the LSC - August 15, 2000 Outline Highlights Meeting Agenda LIGO-G D.
THE INPUT OPTICS OF ENHANCED AND ADVANCED LIGO D.B. Tanner, M.A. Arain, A. Lucianetti, R.M. Martin, V. Quetschke, L.F. Williams, Wan Wu, G. Mueller, and.
LSC meeting, 25/05/07 Thermal lensing simulation 1 Faraday thermal lensing numerical simulations Slim Hamdani EGO LIGO-G Z.
High power fibered optical components for gravitational waves detector Matthieu Gosselin, PhD Student at EGO ELiTES : 3 rd general meeting February 10.
1 Advanced Faraday isolator designs for high average powers. Efim Khazanov, Anatoly Poteomkin, Nikolay Andreev, Oleg Palashov, Alexander Sergeev Institute.
Design for a New Optical Table of the Shintake Monitor Takashi Yamanaka The University of Tokyo ATF2 weekly meeting 2007/9/26.
PXIE absorber test bench A. Shemyakin, C. Baffes, K. Carlson, B. Hanna, L. Prost, J. Walton November 6, 2012 Project X meeting Test bench description Difficulties:
1 1Dr. V.P.Ovsiannikov Cryogenics and vacuum in Dreebit EBITs The vacuum problem in EBIST is the problem of ensuring high vacuum into a long drift tube.
Laser Adaptive Optics for Advanced LIGO
LumiCal High density compact calorimeter at the ILC Wojciech Wierba Institute of Nuclear Physics PAS Cracow, Poland.
Prism Pairs for Elliptical Beams
Advanced Virgo INJ: Faraday isolator, Electro-optical modulator, high power beam dump and Input mode-cleaner E. Genin for AdV INJ team European Gravitational.
Progress toward squeeze injection in Enhanced LIGO
The LIGO input optics D.B. Tanner, M.A. Arain, A. Lucianetti, R. Martin, V. Quetschke, L.F. Williams, Wan Wu, G. Mueller, and D.H. Reitze University.
Commissioning Update PAC 15, Dec. 11, 2003 Daniel Sigg.
Interferometric measurements on mirrors
Modulators and Isolators for
PSL optical layout changes for eLigo
Enhanced LIGO Modulator Supported by NSF grant PHY
Optics Alan Title, HMI-LMSAL Lead,
Drive Laser Commissioning Status
Advanced LIGO R&D Review Input Optics
Fiber End Cap (for high power applications)
Presentation transcript:

G Z 1 eLIGO/advLIGO FI update Antonio Lucianetti, K.L. Dooley, R. Martin, L. F. Williams, M.A. Arain, V. Quetschke, G. Mueller, D.B. Tanner, and D.H. Reitze University of Florida, Gainesville, FL Ligo-Virgo Meeting, Hannover, Oct G R

G Z 2 FI for eLIGO 1 Laser Mod FI GW readout IMC OMC ● High isolation ratio (>30 dB) ● Low beam drift (< 100  rad) ● Weak thermal lens (residual │f│> 30 m) 25 W Current iLIGO FI at Livingston provides an isolation ratio as low as 13.6 dB Refl

G Z 3 eLIGO/advLIGO FI configuration 2 ● Faraday Rotator - Two TGG crystals with a reciprocal QR ● Calcite wedge polarizers (superior to TFPs) ● Thermal lens compensation with - dn/dT material (deuterated dihydrogen phosphate, or ‘DKDP’)

G Z 4 Problems we have encountered TGG and DKDP crystals: - surface damage - improper AR coatings SOLUTION: New vendor (NG) Magnet Diameter ~ 200  m 3 FI magnet ring failure

G Z 5 Characterization of individual TGGs ●Incident laser power: 1 W Result from 6 th order polynomial fit: Max TGG rotation angle (crystal #2): deg +/ deg 4 zz zz

G Z 6 Thermal lens created by TGG and DKDP Telescope Fiber laser beam (1-30 W) DKDP or TGG Focusing lens Beam Scan 5

G Z 7 COMSOL Simulation (radiation enabled on faces and edges) 30 W incident power Time from t = 0s to t = 60s with a line every 1s Parameters: TGG radius = 10.3 mm Laser beam radius = 1.5 mm Temperature in the center of the pumped face (point [0,0,0]) 6 The time constants of thermal lensing are in the order of seconds

G Z 8 30 W incident power Time from t = 0s to t = 3600s (60min) with a line every 60s (1min) Parameters: TGG radius = 10.3 mm Laser beam radius = 1.5 mm Temperature in the center of the pumped face (point [0,0,0]) 7 COMSOL Simulation (radiation enabled on faces and edges)

G Z 9 Faraday Isolator performance Isolation ratio (CWPs) 8 ● Decrease in isolation ratio under vacuum as time went on ● Could be recovered by < 2 degree rotation of waveplate P L = 25W p = 4*10 -6 Torr WP adjusted IR of iLIGO FI (LLO)

G Z 10 Faraday isolator performance Effect of vacuum 9 ● P L = 25 W ● DKDP between CWPs

G Z Faraday isolator performance thermal drift (CWPs) P L = 25W p = 4*10 -6 Torr Result: Over the course of six hrs the horizontal and the vertical intrinsic drifts are < 50 microradians FI

G Z 12 ELIGO FI Schedule LLO ● Assembly, final test and measurements of the FI will be done in the clean optics lab at the LIGO Livingston Observatory ● Installation of the FI for LLO will start on Nov 13, ● Integration and commissioning of the FI and Input Optics with PSL is planned to start on June 3, LHO ● Installation of the FI at LHO is planned to start in December 2007 or January ● Integration and commissioning of the FI and Input Optics with PSL is planned to start on Feb. 19,

G Z 13 Conclusions ● Initial LIGO FI measurements reveal that isolation requirements for E-LIGO are very relaxed → 20 dB will work well ● Obtained 43 dB isolation ratio with CWPs in vacuum Decrease in isolation ratio under vacuum should be recovered by < 2 degree rotation of waveplate. Intrinsic thermal drift of the reflected beam was < 50 microradians for the horizontal and vertical axes ● Performance is expected to improve with Northrop Grumman crystals (TGG/DKDP) and new precision mount for DKDP with tip/tilt positioning