Heavy IMC end payload requirements

Slides:



Advertisements
Similar presentations
19. October 2004 A. Freise Automatic Alignment using the Anderson Technique A. Freise European Gravitational Observatory Roma
Advertisements

Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
Cascina, January 25th, Coupling of the IMC length noise into the recombined ITF output Raffaele Flaminio EGO and CNRS/IN2P3 Summary - Recombined.
Marcus Ng Mentor: Alan Weinstein Co-mentor: Robert Ward
Optics of GW detectors Jo van den Brand
Stefan Hild and Andreas Freise University of Birmingham Advanced Virgo telecon, June 2008 Beam sizes and mirror curvatures for Advanced Virgo.
F. Frasconi I.N.F.N. Pisa for the Virgo Collaboration TAUP2007 Sendai, September 11-15, 2007 VIRGO EXPERIMENT VIRGO: a large interferometer for Gravitational.
rd ILIAS-GW annual general meeting 1 VIRGO Commissioning progress J. Marque (EGO)
1 Gravitational wave interferometer OPTICS François BONDU CNRS UMR 6162 ARTEMIS, Observatoire de la Côte d’Azur, Nice, France EGO, Cascina, Italy May 2006.
Virgo Control Noise Reduction
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,
1 Ist Virgo+ review Cascina H. Heitmann Alignment: Virgo+ changes.
Joshua Smith December 2003 Detector Characterization of Dual-Recycled GEO600 Joshua Smith for the GEO600 team.
Status of LCGT and CLIO Masatake Ohashi (ICRR, The University of TOKYO) and LCGT, CLIO collaborators TAUP2007 Sendai, Japan 2007/9/12.
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.
Design of Stable Power-Recycling Cavities University of Florida 10/05/2005 Volker Quetschke, Guido Mueller.
Intermediate review - ERC – February 9, 2009 – L. Pinard 1 Mirrors Sub-System Overview  Introduction  Scope of the subsystem, main tasks  Job done since.
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.
Stefan Hild October 2007 LSC-Virgo meeting Hannover Interferometers with detuned arm cavaties.
1 1.ISC scope and activities 2.Initial Virgo status 3.Design requirements 4.Reference solution and design status 5.Plans toward completion 6.Technical.
GEO‘s experience with Signal Recycling Harald Lück Perugia,
European Gravitational Observatory12/12/2005 WG1 Hannover 1 Mode Matching of the Fabry-Perrot cavities Julien Marque.
LISA October 3, 2005 LISA Laser Interferometer Space Antenna Gravitational Physics Program Technical implications Jo van.
LIGO-G D The LIGO-I Gravitational-wave Detectors Stan Whitcomb CaJAGWR Seminar February 16, 2001.
LIGO- G R Telecon on June, Mach-Zender interferometer to eliminate sidebands of sidebands for Advanced LIGO Osamu Miyakawa, Caltech.
1 GEO Simulation Workshop, October 25 th 2007 M Laval The Virgo FFT code: DarkF Mikael Laval CNRS UMR 6162 ARTEMIS, Observatoire de la Côte d’Azur, Nice,
G Z AJW for Marcus Benna, Cambridge Wavefront Sensing for Advanced LIGO Model of wavefront sensing in a dual- recycled interferometer Consequences.
Advanced Virgo Optical Configuration ILIAS-GW, Tübingen Andreas Freise - Conceptual Design -
LSC-VIRGO joint meeting - Pisa1 Input mirrors thermal lensing effect Frequency modulation PRCL length in Virgo Some results from a Finesse simulation.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
CALVA : A test facility for Lock Acquisition F.Cavalier 1 on behalf of CALVA team : M.-A.Bizouard 1, V.Brisson 1, M.Davier 1, P.Hello 1, N.Leroy 1, N.Letendre.
1 Advanced Virgo Workshop 14/06/2007 M Laval Fabry Perot cavity for LG and Flat modes Mikael Laval (OCA/ARTEMIS) Outlines: Tools: The optical simulation.
1 Thermal noise and high order Laguerre-Gauss modes J-Y. Vinet, B. Mours, E. Tournefier GWADW meeting, Isola d’Elba May 27 th – Jun 2 nd, 2006.
AIGO 2K Australia - Italy Workshop th October th October 2005 Pablo Barriga for AIGO group.
1st Advanced Virgo Review – November 3-4, 2008 – L. Pinard 1 Mirrors Sub-System Overview  Introduction  Scope of the subsystem, main tasks  Substrates.
Nov 3, 2008 Detection System for AdV 1/8 Detection (DET) Subsystem for AdV  Main tasks and requirements for the subsystem  DC readout  Design for: the.
AdV Thermal Compensation System Viviana Fafone AdV/aLIGO joint technical meeting, February 4, 2004.
Dual Recycling in GEO 600 H. Grote, A. Freise, M. Malec for the GEO600 team Institut für Atom- und Molekülphysik University of Hannover Max-Planck-Institut.
First DR FFT Results on Advanced LIGO Using Perfect and Imperfect Optics By Ken Ganezer, George Jennings, and Sam Wiley CSUDH LIGO-G Z by Ken.
The status of VIRGO Edwige Tournefier (LAPP-Annecy ) for the VIRGO Collaboration HEP2005, 21st- 27th July 2005 The VIRGO experiment and detection of.
Paolo La Penna ILIAS N5-WP1 meeting Commissioning Progress Hannover, July 2004 VIRGO commissioning progress report.
Advanced Virgo: Optical Simulation and Design Advanced Virgo review Andreas Freise for the OSD Subsystem.
Cascina, Nov. 4 th, 2008 AdV review 1 AdV Injection system E. Genin European Gravitational Observatory.
ILIAS - Geneve1 Input mirrors thermal lensing effect in Virgo J. Marque.
Advanced Advanced Virgo BASELINE DESIGN advanced Giovanni Losurdo – INFN Firenze Advanced Virgo Coordinator for the Virgo Collaboration.
The VIRGO detection system
1 ILIAS WG1 meeting, Hannover The 2 nd modulation frequency project.
The Proposed Holographic Noise Experiment Rainer Weiss, MIT On behalf of the proposing group Fermi Lab Proposal Review November 3, 2009.
1 Cascina – October 19, 2011 ASPERA Forum Laurent Pinard Substrates, Polishing, Coatings and Metrology for the 2 nd generation of GW detector Laurent PINARD.
Interferometer configurations for Gravitational Wave Detectors
A look at interferometer topologies that use reflection gratings
Daniel Sigg, Commissioning Meeting, 11/11/16
The Proposed Holographic Noise Experiment
Design of Stable Power-Recycling Cavities
Gravitational wave interferometer OPTICS
Virgo – Injection SYStem
Advanced LIGO Quantum noise everywhere
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
Thermal noise and high order Laguerre-Gauss modes J-Y. Vinet, B
3rd generation ITF sensitivity curve
LIGO Scientific Collaboration
40m TAC Update October 2006 The 40m Team 11 April 2019 G I.
Flat-Top Beam Profile Cavity Prototype
The views of Virgo collaboration groups on upgraded/advanced Virgo
MC radiation pressure effects
Advanced Virgo ISC subsystem
Presentation transcript:

Heavy IMC end payload requirements M.Punturo

Translation of the IMC end mirror Current payload is made in such a way the suspension point can be translated by 11cm in the beam axis direction Motorization Counter-weight (800g) 360g mirror and ~5kg reference mass

February detector meeting P.Puppo shown a possible large payload design able to translate many cm http://wwwcascina.virgo.infn.it/collmeetings/presentations/2006/2006-02/DetectorMeeting/puppo_8Feb_DM.ppt But what are really the true requirements?

Optical Constrains Thanks to: "Measurement of the optical parameters of the Virgo interferometer“ document The same modulation frequency is used both for the longitudinal locking and for the alignment This must be resonant in the recycling and in the mode cleaner cavity The length of these cavities must be matched to the fmod or viceversa For the recycling cavity the phase shift of the FP must be taken in account The use of the Anderson technique for the Angular alignment requires that “the TEM01 mode of the upper sideband is distant from the carrier by an exact number of free spectral range” The Anderson frequency fAnd is the difference between the resonance frequencies of the TEM00 and TEM01 modes and it is univocally defined by the cavity geometry: Reff~Rend mirror The modulation frequency fmod must correspond to the optimal one within the cavity linewidth (Df=500Hz):

Mechanical displacements requirements The optical constrains require a mechanical displacement range smaller than two cm On the contrary, the initial position of the IMC end mirror must be well selected Passing from the current 3 cm thick mirror to a 10 cm thick the reflecting surface advances by 3.5 cm (and similarly the IMC cavity will be shortened by 3.5cm) The suspension point of the new payload must be off-centered to take in account this offset

Conclusion The design of the new heavy payload for the end mirror of the IMC will take in account a displacement system having a range of ±3 cm

Large BS update J.Marque preliminary studies: Very large BS needed to reduce the scattered light Studied geometry is monstrous but what are our limits? L.Pinard contacted Heraeus can produce a 700 mm diameter BS (thickness is a limitation) LMA can coat a mirror larger than 400 mm, but this is the upper limit for the characterization facility J.Marque, Det. Meeting 8-2-2003