LIGO LaboratoryLIGO-G080346-00-R Coatings and Their Influence on Thermal Lensing and Compensation in LIGO Phil Willems Coating Workshop, March 21, 2008,

Slides:



Advertisements
Similar presentations
Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
Advertisements

Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
LIGO Laboratory1 Thermal Compensation Experience in LIGO Phil Willems- Caltech Virgo/LSC Meeting, Cascina, May 2007 LIGO-G Z.
Thermal Compensation System – TCS Technical Presentation aLIGO NSF Review LIGO Livingston Observatory April LIGO-G v5.
LIGO-G W LIGO Scientific Collaboration Meeting – LLO March Summary of recent measurements of g factor changes induced by thermal loading.
LIGO-G W Raab: Searching for Gravitational Waves w/ LIGO1 Why Has Duty Cycle Been Lower in Livingston.
Thermal Compensation NSF David Ottaway LIGO Laboratory MIT.
LIGO-G W 2005 CLEO/QELS Joint Symposium on Gravitational Wave Detection 1 High-Power Stabilized Lasers and Optics of GW Detectors Rick Savage.
LIGO-G9900XX-00-M LIGO R&D1 Gold Coatings in Advanced LIGO Phil Willems.
Thermal Compensation Review David Ottaway LIGO Laboratory MIT.
LIGO-G W 2005 CLEO/QELS Joint Symposium on Gravitational Wave Detection 1 High-Power Stabilized Lasers and Optics of GW Detectors Rick Savage.
Thermally Deformable Mirrors: a new Adaptive Optics scheme for Advanced Gravitational Wave Interferometers Marie Kasprzack Laboratoire de l’Accélérateur.
Stefan Hild, Andreas Freise, Simon Chelkowski University of Birmingham Roland Schilling, Jerome Degallaix AEI Hannover Maddalena Mantovani EGO, Cascina.
LIGO-G D Advanced LIGO Systems Design & Interferometer Sensing & Optics Peter Fritschel, LIGO MIT PAC 13 Meeting, 5 June 2003.
1 G Mike Smith Gravitational Waves & Precision Measurements.
Design of Stable Power-Recycling Cavities University of Florida 10/05/2005 Volker Quetschke, Guido Mueller.
Optical Configuration Advanced Virgo Review Andreas Freise for the OSD subsystem.
Test mass dynamics with optical springs proposed experiments at Gingin Chunnong Zhao (University of Western Australia) Thanks to ACIGA members Stefan Danilishin.
Degeneracy for power-recycling and signal recycling cavities in Advanced Virgo.
1 The Status of Melody: An Interferometer Simulation Program Amber Bullington Stanford University Optics Working Group March 17, 2004 G D.
LIGO-G D LIGO R&D1 Thermal Compensation System Design Requirement and Conceptual Design Review Presentation Phil Willems and Mike Smith August.
Thermal Compensation: The GEO and LIGO experience and requirements for advanced detectors Gregory Harry LIGO/MIT On behalf of the LIGO Science Collaboration.
Thermal Compensation in Stable Recycling Cavity 21/03/2006 LSC Meeting 2006 UF LIGO Group Muzammil A. Arain.
Gravitational Wave Detection Using Precision Interferometry Gregory Harry Massachusetts Institute of Technology - On Behalf of the LIGO Science Collaboration.
LIGO Laboratory1 Enhanced and Advanced LIGO TCS Aidan Brooks - Caltech Hannover LSC-VIRGO Meeting, October 2007 LIGO-G Z.
DFG-NSF Astrophysics Workshop Jun 2007 G Z 1 Optics for Interferometers for Ground-based Detectors David Reitze Physics Department University.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
Advanced Virgo Optical Configuration ILIAS-GW, Tübingen Andreas Freise - Conceptual Design -
Parametric Instabilities and Control Li Ju ( 鞠莉), Chunnnong Zhao, David Blair Jiayi Qin, Qi Fang, Carl Blair, Jian Liu University of Western Australia.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
An Off-Axis Hartmann Sensor for Measurement of Wavefront Distortion in Interferometric Detectors Aidan Brooks, Peter Veitch, Jesper Munch Department of.
AIGO 2K Australia - Italy Workshop th October th October 2005 Pablo Barriga for AIGO group.
Advanced LIGO Simulation, 6/1/06 Elba G E 1 ✦ LIGO I experience ✦ FP cavity : LIGO I vs AdvLIGO ✦ Simulation tools ✦ Time domain model Advanced.
Thermal Compensation System V. Fafone for the TCS Subsystem.
AdV Thermal Compensation System Viviana Fafone AdV/aLIGO joint technical meeting, February 4, 2004.
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.
LSC-Virgo Caltech on March 20, 2008 G E1 AdvLIGO Static Interferometer Simulation AdvLIGO simulation tools  Stationary, frequency domain.
TCS and IFO Properties Dave Ottaway For a lot of people !!!!!! LIGO Lab Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of.
LIGO Laboratory1 Thermal Compensation in LIGO Phil Willems- Caltech Baton Rouge LSC Meeting, March 2007 LIGO-G Z.
ACIGA High Optical Power Test Facility
Aidan Brooks, Peter Veitch, Jesper Munch
17/05/2010A. Rocchi - GWADW Kyoto2 Thermal effects: a brief introduction  In TM, optical power predominantly absorbed by the HR coating and converted.
Advanced Virgo: Optical Simulation and Design Advanced Virgo review Andreas Freise for the OSD Subsystem.
Some considerations on radiative cooling V. Fafone, Y. Minenkov, I. Modena, A. Rocchi INFN Roma Tor Vergata.
LIGO Scientific Collaboration
Thermal Compensation System TCS V. Fafone for the TCS Subsystem.
Hartmann Wavefront Sensing for the Gingin Experiment Aidan Brooks, Peter Veitch, Jesper Munch Department of Physics, University of Adelaide LSC, LLO Mar.
GEO Status and Prospects Harald Lück ILIAS / ETmeeting Cascina November 2008.
LIGO-G D Core Optics Components (COC) Polishing Pathfinder Kickoff Advanced LIGO Project GariLynn Billingsley Caltech.
LIGO-G D Advanced LIGO Systems & Interferometer Sensing & Control (ISC) Peter Fritschel, LIGO MIT PAC 12 Meeting, 27 June 2002.
LIGO-G d April 24, 2007 Auxiliary Optics System (AOS) Technical Breakout Presentation NSF Review of Advanced LIGO Project Mike Smith, Phil Willems.
Thermal compensation issues: sensing and actuation V. Fafone University of Rome Tor Vergata and INFN ASPERA Technological Forum – EGO October, 2011.
Interferometer configurations for Gravitational Wave Detectors
Thermal Compensation NSF
Auxiliary Optics System (AOS)
LIGO Core Optics: a decade of development and experience
Design of Stable Power-Recycling Cavities
Commissioning the LIGO detectors
Thermal lensing and the Gingin test 1
Thermal Compensation System Design Requirement and Conceptual Design Review Presentation Phil Willems and Mike Smith August 17, 2006 LSU LIGO R&D.
Thermal Compensation Installation at LHO
Workshop on Gravitational Wave Detectors, IEEE, Rome, October 21, 2004
Flat-Top Beam Profile Cavity Prototype: design and preliminary tests
Modeling of Advanced LIGO with Melody
Status of the LIGO Detectors
LIGO Scientific Collaboration
Improving LIGO’s stability and sensitivity: commissioning examples
Thermal lensing and the Gingin test 1
Flat-Top Beam Profile Cavity Prototype
Presentation transcript:

LIGO LaboratoryLIGO-G R Coatings and Their Influence on Thermal Lensing and Compensation in LIGO Phil Willems Coating Workshop, March 21, 2008, Caltech

LIGO LaboratoryLIGO-G R Initial LIGO Thermal Compensation CO 2 Laser ? Over-heat correction pattern Inhomogeneous correction pattern Under-heat correction pattern ZnSe viewport

LIGO LaboratoryLIGO-G R Thermal Lensing Phenomena 1: Arm Cavity Mode Shape and Loss Heating in the bulk and coating of the test masses deforms the arm cavity reflective surfaces »Uniform absorption: center heats more than periphery, roughly equivalent to radius of curvature change → cavity mode is still TEM00 but with a different size and waist location Spot Sizes: at small IFO power: 6.0 cm at full IFO power: 5.4 cm

LIGO LaboratoryLIGO-G R Thermal Lensing Phenomena 1: Arm Cavity Mode Shape and Loss »Nonuniform absorption a more open question, but most nonuniformities are strong point absorbers on uniform background→ thermoelastic ‘blisters’ arise, scattering power from the TEM00 mode (‘thermal microroughness’) –Amount of scatter depends on location of spots, substrate choice, and excess absorption –Equal scatter requires ~3x lower absorption per point for fused silica –Compensating this effect in the arm cavity would be heroic and is not planned

LIGO LaboratoryLIGO-G R Thermal Lensing Phenomena 2: RF Sideband Power Buildup Thermal aberrations in substrate (and to lesser extent thermoelastic deformation of surfaces) corrupt RF sidebands in recycling cavities, limiting cavity finesse: Requirement on TC is that RF sideband power not saturate even at full power; in DC readout scheme these sidebands not needed for GW demod. RF power increases linearly with injected power at low power RF power falls at high power due to thermal-lens-induced mismatch

LIGO LaboratoryLIGO-G R Thermal Lensing Phenomena 3: GW Sideband Extraction Efficiency Resonant sideband extraction relies on resonance of gravitational wave sidebands in signal recycling cavity for signal response. Aberrations in signal recycling cavity convert sideband light into sterile higher-order modes. Quantum calculations of RSE spectrum with SRC loss This sets the most severe limit on allowable aberrations; ~0.1% loss from TEM00 mode yields ~5% reduction in sensitivity at high frequencies. (NB: this number applies to older, high-finesse cavity design)

LIGO LaboratoryLIGO-G R Thermal Lensing Phenomena 3: GW Sideband Extraction Efficiency At lower frequencies optical sensitivity is less affected by loss, and thermal noise sets the noise floor. Low frequency sensitivity is far more robust against thermal aberration.

LIGO LaboratoryLIGO-G R Compensator Design: Ring Heater Heating rear face of test mass with any reasonable symmetric configuration causes an ROC correction of front face Ring heaters are used to reduce the test mass ROCs »Static curvature correction »Thermoelastic bump correction

LIGO LaboratoryLIGO-G R Compensator Design: CO 2 Laser Heater CO 2 Laser homogeneous correction pattern ZnSe viewport Compensation Plate Input Test Mass

LIGO LaboratoryLIGO-G R Compensation Sensors Phase cameras »Advantages: –On-axis, no parallax distortion –Sees all aberration in interferometer »Disadvantages: –Separating aberration from individual optics difficult »Currently in use on initial LIGO Off-axis Hartmann sensors »Advantages: –Sees aberration of individual ITMs separately »Disadvantages: –Does not see aberration except in ITMs »Hartmann sensor tested successfully at Gingin

LIGO LaboratoryLIGO-G R How Much Absorption Can We Tolerate? Baseline Advanced LIGO design assumes 0.5 ppm coating absorption Design is required to maintain a power margin of 2 (i.e. 1 ppm would be just tolerable) Why not a margin of 10? »TCS injects noise into the system; the more power, the more noise »TCS injects heat into the mirrors; temperature rise increases thermal stress and thermal noise »TCS injects heat into SUS support structure, which can seize up if overheated (this sets a surprisingly tight requirement) »Larger thermal lenses must be corrected with greater fidelity, which increases the difficulty