Toward a 3rd generation European Gravitational Wave Observatory Dual R&D: presented by Massimo Cerdonio INFN Section and Department of Physics Padova how.

Slides:



Advertisements
Similar presentations
Photon absorption Local heating Thermal expansion INFN-LENS T2 Braginsky et al., Phys. Lett. A 264, 1 (1999) Cerdonio et al., Phys. Rev. D 63, (2001)
Advertisements

Task M2 – Advanced Materials and Techniques for Resonant Detectors Motivation : Reduce thermal noise contribution to the acoustic detector noise budget.
T3 considers two aspects of the thermal noise The problem of the interrogation area of the test mass. Small interrogation area means large fluctuations.
WP-M3 Superconducting Materials PArametric COnverter Detector INFN_Genoa Renzo Parodi.
Design and performance of the Dual detector with large area capacitive readout 4 rd ILIAS-GW Meeting, October 8 th – 9 th 2007, Tuebingen Paolo Falferi.
April 27th, 2006 Paola Puppo – INFN Roma ILIAS Cryogenic payloads and cooling systems (towards a third generation interferometer) part II: the Vibration.
Dual Sphere Detectors by Krishna Venkateswara. Contents  Introduction  Review of noise sources in bar detectors  Spherical detectors  Dual sphere.
1st ET General meeting, Pisa, November 2008 The ET sensitivity curve with ‘conventional‘ techniques Stefan Hild and Andreas Freise University of Birmingham.
Mechanical amplifiers for the DUAL detector: lumped and distributed element design 3 rd ILIAS-GW Meeting, October 26 th – 27 th 2006, London Paolo Falferi.
ILIAS meeting Mallorca 2005 V. Fafone Viviana Fafone INFN - LNF Future plans for resonant detectors
An optomechanical transducer for the AURIGA “bar” gw detector cryogenic optics towards the quantum limit: high finesse cavities, fibers, piezo actuators,
TeV Particle Astrophysics August 2006 Caltech Australian National University Universitat Hannover/AEI LIGO Scientific Collaboration MIT Corbitt, Goda,
Towards a Design Study Proposal for a 3rd Generation Interferometric Gravitational- wave Detector Harald Lück London, October 26th 2006.
Recent Developments toward Sub-Quantum-Noise-Limited Gravitational-wave Interferometers Nergis Mavalvala Aspen January 2005 LIGO-G R.
GWADW, May 2012, Hawaii D. Friedrich ICRR, The University of Tokyo K. Agatsuma, S. Sakata, T. Mori, S. Kawamura QRPN Experiment with Suspended 20mg Mirrors.
GWADW 2010 in Kyoto, May 19, Development for Observation and Reduction of Radiation Pressure Noise T. Mori, S. Ballmer, K. Agatsuma, S. Sakata,
LISA STUDIES AT THE UNIVERSITY OF COLORADO Michael J. Nickerson, Ellery B. Ames, John L. Hall, and Peter L. Bender JILA, University of Colorado and NIST,
Auriga, Explorer and Nautilus Eugenio Coccia INFN Gran Sasso and U. of Rome “Tor Vergata” GWADW Elba 2006.
Acoustic gw detectors: from resonant “bar” to wideband “dual” AURIGA DUAL R&D Erice June 3 rd 2006 Massimo.
Optical readout for a resonant gw bar. Old setup.
STREGA WP1/M1 mirror substrates GEO LIGO ISA Scientific motivation: Mechanical dissipation from dielectric mirror coatings is predicted to be a significant.
CNRS LKB – Task T1 Current status of the experiment on optomechanical coupling Sensitivity: 5.10  20 m.Hz  1/2   New high-finesse, high-power cavity.
1 Paolo Falferi - ET WG2 meeting - Glasgow, 22/7/2010 Actuator magnetic noise measurement and possible developments Paolo Falferi CNR-FBK Trento and INFN.
Summary and Plans for the WG3 activity H.Lück, M.Punturo.
Design study for ET 3rd generation Gravitational Wave Interferometer Work Package 2 Suspension, Thermal noise and Cryogenics Piero Rapagnani
GWDAW 9 - December 15 th, 2004 STATUS OF EXPLORER AND NAUTILUS INFN – LN Frascati, LN Gran Sasso, Sez. Roma 1, Roma 2 and Genova Universities “La Sapienza”
Optomechanical Devices for Improving the Sensitivity of Gravitational Wave Detectors Chunnong Zhao for Australian International Gravitational wave Research.
SQL Related Experiments at the ANU Conor Mow-Lowry, G de Vine, K MacKenzie, B Sheard, Dr D Shaddock, Dr B Buchler, Dr M Gray, Dr PK Lam, Prof. David McClelland.
New materials for DUAL: the LNL activity. Dual detector : Best material parameters Two different materials ‘A’ and ‘B’ with two different Young modulus.
LISA October 3, 2005 LISA Laser Interferometer Space Antenna Gravitational Physics Program Technical implications Jo van.
New Low-Frequency GW Detector with Superconducting Instrumentation
INTERPRETATION of IGEC RESULTS Lucio Baggio, Giovanni Andrea Prodi University of Trento and INFN Italy or unfolding gw source parameters starting point:
JRA3 STREGA - Introduction Geppo Cagnoli IGR – University of Glasgow ILIAS-GW Meeting, Orsay, 5 th -6 th Nov 2004.
The AURIGA experiment: updates and prospects BAGGIO Lucio ICRR on behalf of AURIGA collaboration The AURIGA detector re-started data taking in Dec 2003,
PeTeR: a hardware simulator for LISA PF TM-GRS system 23/05/ th LISA Symposium May 2012, BnF Paris L. Marconi and R. Stanga Università degli.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
Task M2 – Working group Auriga-LNL Operation temperature KOperation temperature K Mechanical Attenuation >180dB in the frequency range.
Quantum noise observation and control A. HeidmannM. PinardJ.-M. Courty P.-F. CohadonT. Briant O. Arcizet T. CaniardJ. Le Bars Laboratoire Kastler Brossel,
Cold damping of fused silica suspension violin modes V.P.Mitrofanov, K.V.Tokmakov Moscow State University G Z.
Giovanni Andrea Prodi University of Trento and INFN Italy 2 nd GWPW, Penn State, Nov.6 th, 2003 IGEC observations in : exchanged data multiple.
R&D on thermal noise in Europe: the STREGA Project Geppo Cagnoli University of Glasgow AMALDI 6 – Okinawa - Japan June
Wideband acoustic gravitational wave detectors at kHz frequencies: from AURIGA to DUAL AURIGA Caltech Dec 12 th 2005 Massimo Cerdonio.
Parametric Instabilities In Advanced Laser Interferometer Gravitational Wave Detectors Li Ju Chunnong Zhao Jerome Degallaix Slavomir Gras David Blair.
Thermoelastic dissipation in inhomogeneous media: loss measurements and thermal noise in coated test masses Sheila Rowan, Marty Fejer and LSC Coating collaboration.
Investigation of effects associated with electrical charging of fused silica test mass V. Mitrofanov, L. Prokhorov, K. Tokmakov Moscow State University.
Gravitational Experiment Below 1 Millimeter and Search for Compact Extra Dimensions Josh Long, Allison Churnside, John C. Price Department of Physics,
WG3 Report Michele Punturo Harald Lück. WG3 composition Co-Chairmen M.Punturo INFN Perugia, Italy H.Lück MPI für Gravitationsphysik, AEI, Hannover, Germany.
SQL Related Experiments at the ANU Conor Mow-Lowry, G de Vine, K MacKenzie, B Sheard, Dr D Shaddock, Dr B Buchler, Dr M Gray, Dr PK Lam, Prof. David McClelland.
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,
1/16 Nawrodt, Genoa 09/2009 An overview on ET-WP2 activities in Glasgow R. Nawrodt, A. Cumming, W. Cunningham, J. Hough, I. Martin, S. Reid, S. Rowan ET-WP2.
G. Cella I.N.F.N. Sezione di Pisa.  The mass density fluctuates..... ..... and the gravitational field will do the same Direct gravitational coupling.
1 The control of the Virgo mirrors is realized using coil-magnet actuators Can this technique be used in ET, from room to cryogenic temperatures? Is the.
Status of AURIGA AURIGA Sept 21 st 2005 Massimo Cerdonio INFN Section and Department of Physics University of Padova,
Active Vibration Isolation using a Suspension Point Interferometer Youichi Aso Dept. Physics, University of Tokyo ASPEN Winter Conference on Gravitational.
Department of Physics & Astronomy Institute for Gravitational Research Scottish Universities Physics Alliance Brownian thermal noise associated with attachments.
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY Violin-Mode Detector N.A. Lockerbie and K.V. Tokmakov Hannover 27 January, 2010.
Metallurgha.ir1. Lecture 5 Advanced Topics II Signal, Noise and Bandwidth. Fundamental Limitations of force measurement metallurgha.ir2.
Ho Jung Paik University of Maryland GW Astronomy, Korea August, 2016
Amplitude and time calibration of the gw detector AURIGA
Mechanical Loss in Silica substrates
Wide Bandwidth Dual Acoustic GW Detectors
Overview of quantum noise suppression techniques
Nergis Mavalvala Aspen January 2005
Advanced LIGO Quantum noise everywhere
Renzo F. Parodi INFN-Genova
Newtonian Noise Mitigation by Using Superconducting Gravity Gradiometers Ho Jung Paik Department of Physics University of Maryland ICGAC-XIII, Seoul.
Structural analysis of the SOGRO platform
T3 DEVELOPMENT OF SELECTIVE READOUT SCHEMES
Advanced Optical Sensing
The ET sensitivity curve with ‘conventional‘ techniques
Presentation transcript:

Toward a 3rd generation European Gravitational Wave Observatory Dual R&D: presented by Massimo Cerdonio INFN Section and Department of Physics Padova how to obtain the best from acoustic detectors the DUAL R&D collaboration: Firenze, Legnaro, Padova, Trento, Urbino talk prepared by Michele Bonaldi IFN-CNR and INFN, Trento

Toward a 3rd generation European Gravitational Wave Observatory M = 2.3 t L = 3m Resonant bar detectors were designed in late 80’s

Toward a 3rd generation European Gravitational Wave Observatory Used to improve suspension system design Wideband readout design New devices and methods are now available Superconductive amplifier sensitivity improved by a factor of 100 Optical readout for acoustic detectors Methods to develop large masses (100 ton) New high cross section materials Readout systems: FEM analysis: Test masses:

Toward a 3rd generation European Gravitational Wave Observatory When applied to AURIGA: Shh 1st run ( ) 2th run ( )

Toward a 3rd generation European Gravitational Wave Observatory Superconductive amplifier sensitivity improved by a factor of 100 P. Falferi et al., Appl. Phys. Lett. 82, 931 (2003) Optical readout available for acoustic detectors L. Conti et al., J. Appl. Phys. 93 (2003) 3589 Readout systems:

Toward a 3rd generation European Gravitational Wave Observatory Suspension system design - M. Bignotto, Rev. Sci. Instrum. 76, (2005) FEM analysis: 3 - mode readout (100 Hz BW) L.Baggio et al, Phys. Rev. Lett. 94, (2005)

Toward a 3rd generation European Gravitational Wave Observatory Technical improvement is not enough! DUAL detector is based on new ideas 1 – Wideband transducer: read displacement signal between two massive resonator - M. Cerdonio et al. Phys. Rev. Lett (2001) 2 - Selective readout: only GW sensitive normal modes must be measured - M. Bonaldi et al. Phys. Rev. D (2003) Avoid resonant bandwidh limit and thermal noise contribution by the resonant transducer Reduce overall thermal noise by rejecting the contribution of not useful modes

Toward a 3rd generation European Gravitational Wave Observatory Measurement of differential deformations of two nested resonators Intermediate GW broadband Dual: Main Concept 5.0 kHz π Phase difference The inner resonator is driven below frequency The outer resonator is driven above resonance

Toward a 3rd generation European Gravitational Wave Observatory Mode selection strategy 2-D Quadrupolar filter: X=X 1 +X 3 –X 2 –X 4 Capacitive transducer design Large interrogation regions Geometrically based mode selection Reject high frequency resonant modes which do not carry any GW signal Bandwidth free from acoustic modes not sensitive to GW Also FFP optical scheme F. Marin et.al, Phys. Lett. A 309, 15 (2003)

Toward a 3rd generation European Gravitational Wave Observatory Mo Dual 16.4 ton height 3.0m 0.94m SiC Dual 62.2 ton height 3.0m 2.9m Q/T=2x10 8 K -1 M. Bonaldi et al. Phys. Rev. D (2003) Evaluated sensitivity (SQL)

Toward a 3rd generation European Gravitational Wave Observatory Dual R&D : 3 main research topics Detector design seismic noise control external passive + embedded active displacement sensitivity and wide sensing area underground operation not necessary define requirements mechanical amplification resonant not resonant 15 x 10x 100 Hz BW 4 kHz BW Current technology DUAL requirements high cross section (  v s 2-3 ) Al 5056 Mo, SiC, Sapph. (50 x) Readout system: Test masses: 5x m 5x (100x)

Toward a 3rd generation European Gravitational Wave Observatory Broadband amplification up to 5.0 kHz Displacement gain factor about 10 Negligible intrinsic thermal noise Compliance Leverage type amplifier H.J. Paik, proceedings First AMALDI Conference (1995) Readout system for DUAL: mechanical amplification stage

Toward a 3rd generation European Gravitational Wave Observatory Leverages for optical and capacitive readouts Capacitive readout Electric Field Optical readout 3 Joints Fabry-Perot mirrors 4 paired joints Gain= mm

Toward a 3rd generation European Gravitational Wave Observatory A test-oscillator play the role of a GW detector test mass: First experiment: leverage with optical readout Material Al 7075 Geometrical Gain factor 1/  =10 First Longitudinal mode at 2100 Hz Stiffness K=1.5  10 7 N/m Test-Oscillator: Material Al 7075 First Longitudinal mode at 1800 Hz Stiffness K=3.5  10 8 N/m Effective mass M=5.6 kg Rigid Lever Optimized by a parametric software

Toward a 3rd generation European Gravitational Wave Observatory Mechanical gain measurements Direct Gain = Δy/ Δx Frequency shift Leverage behavior

Toward a 3rd generation European Gravitational Wave Observatory Next step: measure the thermal noise ANSYS Prediction by using Fluctuation Dissipation Theorem T=300 K, Q=10 4, Al 7075, w 0 =365  m Leverage behavior: scaling with 1/ α 1/α

Toward a 3rd generation European Gravitational Wave Observatory Progress towards a wide area optical readout Usual cm-long cavities have small spot size (  1mm) → higher order acoustic modes of the real system contribute to the noise M1 M2 M3 M4 D Phys. Lett. A 309, 15 (2003) To average out the noise, we need a spot size > 10 cm !!!! Folded Fabry-Perot: FFP relative shot noise limited displacement sensitivity: constant relative freq. noise due to Brownian noise  1/ N relative freq. noise due to rad pressure noise  1/N 2 + spatial correlation effects effective increase of spot size

Toward a 3rd generation European Gravitational Wave Observatory Progress towards an high sensitivity capacitive readout SQUID amplifiers with sensitivity approaching the quantum limit New SQUID chip design for: - improvement of the energy resolution - reduction of the 1/f noise contribution - suppression of the "hot electron effect" - reduction of the squid losses

Toward a 3rd generation European Gravitational Wave Observatory Apparatus for High voltage breakdown study Bias voltage in the 100 MV/m range M. Bonaldi, F. Penasa, Trento Phys. Dept. Goal: 10 8 V/m Achieved: 10 7 V/m Measurement of V.B. of aluminum polished surfaces of cylindrical samples Two axis adjustment - surface finishing effect - electrodes conditioning procedure - effect of dielectric films Linear vertical stage

Toward a 3rd generation European Gravitational Wave Observatory Test mass material characterization Low temperature measurements of the Q factor of ceramic materials J.P. Zendri, Laboratori Legnaro

Toward a 3rd generation European Gravitational Wave Observatory a deep revision of the resonant detector design The reserch is currently funded by: EGO (R&D program) CNR (QL-READOUT) INFN (DUAL R&D) EC (STREGA) DUAL is based on AND a challenging R&D on readout systems Timeline Feasibility study: Detailed design (?):