Update on Activities in Suspensions for Advanced LIGO Norna A Robertson University of Glasgow and Stanford University LSC meeting, Hanford, Aug 20 th 2002.

Slides:



Advertisements
Similar presentations
Laser Interferometer Gravitational-wave Detectors: Advancing toward a Global Network Stan Whitcomb LIGO/Caltech ICGC, Goa, 18 December 2011 LIGO-G v1.
Advertisements

T1 task- update Mike Plissi. 2 Collaboration Groups actively involved INFN-VIRGO MAT IGR-Glasgow Groups that have expressed interest INFN-AURIGA CNRS-LKB.
Participants: C-1:Cryogenic last-stage suspensions (interferometers) (F.Ricci-G.Frossati) Objectives: -Design new suspension elements for the last stage.
LIGO-G PLIGO Laboratory 1 Advanced LIGO The Next Generation Philip Lindquist, Caltech XXXVIII Moriond Conference Gravitational Waves and Experimental.
G R LIGO Laboratory1 Advanced LIGO Research and Development David Shoemaker LHO LSC 11 November 2003.
Takanori Sekiguchi Italy-Japan Workshop (19 April, 2013) Inverted Pendulum Control for KAGRA Seismic Attenuation System 1 D2, Institute for Cosmic Ray.
LIGO-G D Suspensions Update: the View from Caltech Phil Willems LIGO/Caltech Livingston LSC Meeting March 17-20, 2003.
Silica Research in Glasgow Gianpietro Cagnoli – IGR - University of Glasgow GEO Collaboration Ginzton Lab, Stanford Caltech.
Review of HAM Suspension Designs for Advanced LIGO Norna A Robertson HAM Isolation Requirements Review Caltech, July 11th 2005.
G M Advanced R&D1 Seismic Isolation Retrofit Plan for the LIGO Livingston Observatory Dennis Coyne 29 Nov 2001.
LIGO-G D 1 Requirements Environment and constraints Performance requirements Functional requirements.
LIGO-G M Status of LIGO Barry Barish PAC Meeting Caltech 3-June-04 Upper limits on known pulsar ellipticities.
LIGO-G D Suspensions Design for Advanced LIGO Phil Willems NSF Review, Oct , 2002 MIT.
Active Seismic Isolation Systems for Enhanced and Advanced LIGO Jeffrey S. Kissel 1 for the LSC 1 Louisiana State University The mechanical system for.
Overview of Advanced LIGO March 2011 Rencontres de Moriond Sheila Rowan For the LIGO Scientific Collaboration.
LIGO-G D 1 25-May-02 Advanced LIGO Suspension Model in Mathematica Gravitational Wave Advanced Detector Workshop Elba - May 2002 Mark Barton.
GWADW 2010 in Kyoto, May 19, Development for Observation and Reduction of Radiation Pressure Noise T. Mori, S. Ballmer, K. Agatsuma, S. Sakata,
Advanced LIGO: our future in gravitational astronomy K.A. Strain for the LIGO Science Collaboration NAM 2008 LIGO-G K.
SUSPENSION DESIGN FOR ADVANCED LIGO: Update on GEO Activities Norna A Robertson University of Glasgow for the GEO 600 suspension team LSC Meeting, Louisiana,
Conceptual Design for Advanced LIGO Suspensions Norna A Robertson University of Glasgow and Stanford University for the GEO suspension team +contribution.
1 LIGO and GEO Developments for Advanced LIGO Sheila Rowan, Stanford University/Univ. of Glasgow on behalf of the LIGO Scientific Collaboration APS Annual.
G M 1 Advanced LIGO Update David Shoemaker LSC/Virgo MIT July 2007.
Status of LIGO Data Analysis Gabriela González Department of Physics and Astronomy Louisiana State University for the LIGO Scientific Collaboration Dec.
Update on Advanced LIGO suspension design and technology development towards the quad noise prototype Caroline A. Cantley for Advanced LIGO Suspension.
Advanced LIGO Suspension Status Caroline A. Cantley Advanced LIGO Suspension Team / University of Glasgow for the GEO600 Group LSC Meeting, LLO March 2004.
LIGO-G M Major International Collaboration in Advanced LIGO R&D Gary Sanders NSF Operations Review Hanford February, 2001.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
SUSPENSION DESIGN FOR ADVANCED LIGO: Update on GEO Activities Norna A Robertson University of Glasgow for the GEO 600 suspension team LSC Meeting, Hanford.
G R LIGO Laboratory1 Advanced LIGO David Shoemaker NSF LIGO Review 23 October 2002.
Simulation for KAGRA cryogenic payload: vibration via heat links and thermal noise Univ. Tokyo, D1 Takanori Sekiguchi.
David Shoemaker Aspen 3 February 03
18 th - 22 nd May 2015 LIGO-G GWADW Alaska Suspension Upgrades: Discussion Points + Questions Giles Hammond (Institute for Gravitational Research,
Update on Suspension Activities for Advanced LIGO Caroline A. Cantley University of Glasgow for the GEO600 Group LSC Meeting, Livingston, March 2003 (Technical.
18 th - 22 nd May 2015 LIGO-G GWADW Alaska Suspension Upgrades for Enhanced Interferometers Giles Hammond (Institute for Gravitational Research,
LCGT Technical Review Suspension Point Interferometer for Parasitic Noise Reduction and an Additional IFO S.Miyoki (ICRR, Univ. of TOKYO)
LIGO-G D What can we Expect for the “Upper Limit” Run Stan Whitcomb LSC Meeting 13 August 2001 LIGO Hanford Observatory A Personal Reading of.
Prototype Quadruple Pendulum Update – Part 1 Norna Robertson and Calum Torrie University of Glasgow for the GEO 600 suspension team LSC Meeting, Hanford,
Thermal Noise performance of advanced gravitational wave detector suspensions Alan Cumming, on behalf of the University of Glasgow Suspension Team 5 th.
Advanced LIGO Status Report
LIGO-G M LIGO Status Gary Sanders GWIC Meeting Perth July 2001.
Advanced LIGO UK 1 IGRQA0003 LIGO-G K Modal testing facility for Advanced LIGO Caroline Cantley University of Glasgow Advanced LIGO SUS Workshop,
LIGO-G M Overview of LIGO R&D and Planning for Advanced LIGO Detectors Gary Sanders NSF R&D Review Caltech, January 29, 2001.
Advanced LIGO UK 1 LIGO-G Z Development issues for the UK Advanced LIGO project Caroline Cantley Glasgow University for the UK Advanced LIGO Team.
LSC Meeting March ‘07 1 LIGO ADVANCED SYSTEMS TEST INTERFEROMETER (LASTI) LASTI Progress and Plans LSC Meeting, LLO Dave Ottaway/Richard Mittleman March.
2009/6/25Amaldi 8 in NewYork City1 Thermal-noise-limited underground interferometer CLIO Kazuhiro Agatsuma and CLIO Collaborators Institute for Cosmic.
LIGO-G M Overview of the LIGO Continuing Operations (FY FY2006) Proposal Gary Sanders LIGO PAC9 Meeting December 2000.
G R Advanced LIGO1 David Shoemaker LLO LSC 19 Aug 2002.
LIGO-G Z Silicon as a low thermal noise test mass material S. Rowan, R. Route, M.M. Fejer, R.L. Byer Stanford University P. Sneddon, D. Crooks,
Advanced LIGO UK 1 LIGO-G K OSEM Development UK Advanced LIGO project Stuart Aston University of Birmingham for the UK Advanced LIGO Team LSC.
ALIGO 0.45 Gpc 2014 iLIGO 35 Mpc 2007 Future Range to Neutron Star Coalescence Better Seismic Isolation Increased Laser Power and Signal Recycling Reduced.
LIGO G PLIGO Laboratory 1 Advanced LIGO The Next Generation Philip Lindquist, Caltech XXXVIII Moriond Conference Gravitational Waves and Experimental.
Active Vibration Isolation using a Suspension Point Interferometer Youichi Aso Dept. Physics, University of Tokyo ASPEN Winter Conference on Gravitational.
ALIGO Monolithic stage Giles Hammond, University of Glasgow for the Advanced LIGO Suspensions Team aLIGO/aVirgo Workshop Pisa, Italy 23 rd -24 th February.
LIGO-G D Advanced LIGO Systems & Interferometer Sensing & Control (ISC) Peter Fritschel, LIGO MIT PAC 12 Meeting, 27 June 2002.
Overview of monolithic suspension work for Advanced LIGO Mariëlle van Veggel, Mark Barton, Tim Bodiya, Alan Cumming, Liam Cunningham, Giles Hammond, Gregg.
G R 2004 Plan Update LIGO Systems meeting 22 Jan 04 dhs.
Yoichi Aso Columbia University, New York, NY, USA University of Tokyo, Tokyo, Japan July 14th th Edoardo Amaldi Conference on Gravitational Waves.
LIGO LAB R&D PROGRAM TECHNICAL REVIEW, OCT 02
Advanced Detector Status Report and Future Scenarios
Current and future ground-based gravitational-wave detectors
LCGT Seismic Attenuation System LCGT-SAS
BSC HEPI Pier Amplification
Advanced LIGO Quad Prototype Janeen Romie LSC, March 2004
Advanced VIRGO Experiment
S. Rowan, M. Fejer, E. Gustafson, R. Route, G. Zeltzer
Jim Hough for the GEO collaboration
David Shoemaker AAAS Conference 17 February 2003
Stan Whitcomb LSC meeting Hanford 15 August 2005
HAM SAS Test Plan at LASTI
Characterisation of the aLIGO monolithic suspensions
Presentation transcript:

Update on Activities in Suspensions for Advanced LIGO Norna A Robertson University of Glasgow and Stanford University LSC meeting, Hanford, Aug 20 th 2002 (Plenary Instrument Science Session) DCC Number: LIGO-G Z

Summary of Topics GEO (UK) PPARC proposal for funding for Advanced LIGO Quadruple pendulum design update – with particular reference to low-frequency cut-off Active and eddy current damping of suspensions

GEO (UK) PPARC Proposal for Advanced LIGO Proposal for funding submitted to Particle Physics and Astronomy Research Council (PPARC) for contribution to Advanced LIGO Total requested ~ £ 8.8 million, (~$12M) to supply Advanced LIGO with Technologically advanced suspension systems based on GEO designs Electronic sensing/actuation systems for control Sapphire blanks for test masses for one interferometer Builds on UK experience in gravitational waves research and in particular in GEO Directly involves several UK groups Glasgow University Rutherford Appleton Laboratory (RAL) Birmingham University

PPARC Proposal: Organisational Plan

PPARC Proposal: Roles of Groups Glasgow: overall science management, “problem solving”, scientific support through installation and commissioning, optical material procurement RAL: overall project management, develop final designs and manufacture 28 BSC suspensions (including noise prototypes), participate in installation of LASTI noise prototypes and first 2 units at each site Birmingham: design and supply analogue electronics for local control and global control for all suspensions (HAM and BSC) ~1000 channels All in close collaboration with LIGO Lab

PPARC Proposal - Status Proposal submitted end June 2002 Site visit to Glasgow by review committee 29/30 July 2002 Site visit to Birmingham (date not yet fixed) Proposal goes to Projects Peer Review Panel for consideration in December 2002 Funding requested to start Oct 2003 for 5 years

6 DOF “quiet hydraulics” 2 stage active isolation Update on Quadruple Pendulum Design for Advanced LIGO penultimate mass test mass quadruple pendulum Overall Suspension and Isolation System BSC Chamber

Quadruple Pendulum Design Conceptual design as presented at MARCH LSC meeting: Test mass: 40 kg sapphire, 31.4 cm x 13 cm Penultimate mass: 72 kg (heavy glass) Overall length: 1.7 m (from top blade to centre of mirror) Ribbons : length 60 cm, X-section 113  m x 1.13 mm, stress 770 MPa Highest vert. mode ~8 Hz, first violin mode ~490 Hz

Update on Quadruple Pendulum Design contd Since March LSC meeting, recommendations in document “Low-frequency Cutoff for Advanced LIGO” (DCC T D) have been accepted:- highest vertical mode frequency at 12 Hz or lower violin mode fundamental frequency at 400 Hz or higher horizontal thermal noise specified at 10^-19 m/  Hz or lower at 10 Hz, per test mass technical noise sources (including local damping) at level to allow observations down to 10 Hz. => implications for quad design

Update on Quadruple Pendulum Design contd. Possible changes to conceptual design No requirement for further development of ultra dense (~7 g/cc) heavy glass for penultimate mass Use sapphire or SF4 (heavy glass w/ density 4.8 g/cc) – highest vertical mode ~ 9 Hz, or Use silica – highest vertical mode ~10.4 Hz Consider increasing fibre length to allow use of silica with vert. mode 400 Hz e.g. 70 cm – vert mode 9.6 Hz, violin mode 420 Hz - has consequences for manufacturability, overall length (installation and accommodation in BSC chambers)

Damping of Pendulum Modes Final bullet from “cutoff” recommendations “Technical noise sources (including local damping) at level to allow observations down to 10Hz” Difficult requirement for local damping! typical shadow sensors 10^-10 m/  Hz, range 1 mm mechanical isolation -sensed point to mirror 10 Hz target sensitivity 10^-19 m /  10Hz Possible courses of action After acquisition of lock, use interferometric global sensing as signals for damping – for longitudinal pitch and yaw Develop better sensor, possibly combination coarse/fine sensor Use eddy current damping

Eddy Current Damping Tests at Glasgow Set up on GEO prototype triple pendulum Two 4x4 NdFeB magnet arrays mounted on uppermost mass for investigating vertical and longitudinal damping Magnet array moves within Cu block with corresponding array of holes Damping constant b ~ 5 N / (m s^-1) per array Vertical damping investigated to date (Mike Plissi et al, Glasgow) Cu block magnet array

Eddy Current Damping Tests at Glasgow contd MATLAB Model Vertical transfer function from “ground” to uppermost mass with damping Two peaks: vertical modes at ~ 1Hz (Q~26,) and ~3.5 Hz (Q~13) Upper peak: Q lower than expected from model: - appears to be two modes close together (vertical and pitch) Experimental results undamped

Eddy Current and Active Damping - Conclusions First results + modeling indicate triple pendulums can be adequately damped using eddy currents modecleaners with single arrays (per degree of freedom) heavier recycling mirrors with ~ 3 such arrays Quadruple pendulum requires damping force ~ 20 times a single array. use better conductor for block (e.g. Be) + cooling with peltiers ? General Conclusion Pursue research on both active and eddy current damping