G O D D A R D S P A C E F L I G H T C E N T E R 1 GW Interferometry at Goddard Space Flight Center Jordan Camp NASA / Goddard Space Flight Center Jan.

Slides:



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

LISA Benchtop Experiment at UF Guido Mueller University of Florida 21 st July 2005.
Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
Department ArtemisObservatoire de la Cote d'Azur1 A Sagnac interferometer with frequency modulation for sensitive saturated absorption (and applications.
Dennis Ugolini, Trinity University Bite of Science Session, TEP 2014 February 13, 2014 Catching the Gravitational Waves.
Laser Interferometer Gravitational-wave Detectors: Advancing toward a Global Network Stan Whitcomb LIGO/Caltech ICGC, Goa, 18 December 2011 LIGO-G v1.
Advanced Gravitational-wave Detectors and LIGO-India
T1 task- update Mike Plissi. 2 Collaboration Groups actively involved INFN-VIRGO MAT IGR-Glasgow Groups that have expressed interest INFN-AURIGA CNRS-LKB.
Cryogenic Cavity for Ultra Stable Laser
G v1Advanced LIGO1 Status of Ground-Based Gravitational-wave Interferometers July 11, 2012 Daniel Sigg LIGO Hanford Observatory Astrod 5, Bangalore,
LIGO-G W Is there a future for LIGO underground? Fred Raab, LIGO Hanford Observatory.
Laser Interferometer Space Antenna Satellite Description  Three spacecrafts forming a triangle flying 5 million km apart  Placed in an elliptical plain.
Habitable Planets Astronomy 315 Professor Lee Carkner Special Topic.
The Next 25(?) Years Future Missions to Search for Extra-solar Planets and Life.
1 Observing the Most Violent Events in the Universe Virgo Barry Barish Director, LIGO Virgo Inauguration 23-July-03 Cascina 2003.
Overview Ground-based Interferometers Barry Barish Caltech Amaldi-6 20-June-05.
Teória relativity začiatok alebo koniec fyziky.
1 Institute for Gravitational Research Director: Jim Hough + 4 Academic Staff (Norna Robertson, Harry Ward, Ken Strain, Geppo Cagnoli) + Joint academic.
Current progress of developing Inter-satellite laser interferometry for Space Advanced Gravity Measurements Hsien-Chi Yeh School of Physics Huazhong University.
Katrin Dahl for the AEI 10 m Prototype team March 2010 – DPG Hannover Q29.1 Stabilising the distance of 10 m separated.
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,
1 LISA Science and Concept Robin T. Stebbins. 2 May 13, 2003 LISA Overview The Laser Interferometer Space Antenna (LISA) is a joint ESA- NASA mission.
LIGO-G W Is there a future for LIGO underground? Fred Raab, LIGO Hanford Observatory.
What are GW’s ?? Fluctuation in the curvature of space time, propagating outward form the source at the speed of light Predicted by Einstein’s GTR Gravitational.
Status of LCGT and CLIO Masatake Ohashi (ICRR, The University of TOKYO) and LCGT, CLIO collaborators TAUP2007 Sendai, Japan 2007/9/12.
Thermal noise issues Chinyere Ifeoma Nwabugwu Louisiana State University August 05, 2005 Eric Black, Akira Villar, Kenneth G. Libbrecht, Kate Dooley, Royal.
Advanced LIGO: our future in gravitational astronomy K.A. Strain for the LIGO Science Collaboration NAM 2008 LIGO-G K.
The GEO 600 Detector Andreas Freise for the GEO 600 Team Max-Planck-Institute for Gravitational Physics University of Hannover May 20, 2002.
Interferometer Control Matt Evans …talk mostly taken from…
08/31/2006 ~ Mission specific challenges: Data Analysis GRS Interferometry.
LIGO-G D Enhanced LIGO Kate Dooley University of Florida On behalf of the LIGO Scientific Collaboration SESAPS Nov. 1, 2008.
T1 task- update Mike Plissi. 2 Motivation  Thermo-elastic noise is higher than the ‘intrinsic’ noise in crystalline materials  There are several sources.
The Big Bang Observer: High Laser Power for Gravitational- wave Astrophysics Gregory Harry, Peter Fritschel LIGO Laboratory, Massachusetts Institute of.
GEO600 Detector Status Harald Lück Max-Planck Institut für Gravitationsphysik Institut für Atom- und Molekülphysik, Uni Hannover.
LIGO-G D “First Lock” for the LIGO Detectors 20 October 2000 LIGO Hanford Observatory Stan Whitcomb.
Gravitational Wave Detection Using Precision Interferometry Gregory Harry Massachusetts Institute of Technology - On Behalf of the LIGO Science Collaboration.
Lisbon, 8 January Research and Development for Gravitational Wave Detectors Raffaele Flaminio CNRS/LMA Lyon.
Extra-terrestrial life: Is there anybody out there? Dr Martin Hendry University of Glasgow Reach for the Stars.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
Extrasolar Planets The Search For Ever since humans first gazed into the night sky, the question of whether we are alone in the universe has remained unanswered.
The Search for Extra-Solar Planets Dr Martin Hendry Dept of Physics and Astronomy.
Masaki Ando, Akiteru Takamori, Kimio Tsubono Department of Physics, University of Tokyo Earthquake Research Institute, University of Tokyo 1st International.
Abstract The Hannover Thermal Noise Experiment V. Leonhardt, L. Ribichini, H. Lück and K. Danzmann Max-Planck- Institut für Gravitationsphysik We measure.
LIGO LaboratoryLIGO-G R Coatings and Their Influence on Thermal Lensing and Compensation in LIGO Phil Willems Coating Workshop, March 21, 2008,
Update on Activities in Suspensions for Advanced LIGO Norna A Robertson University of Glasgow and Stanford University LSC meeting, Hanford, Aug 20 th 2002.
Structure Formation in the Universe Concentrate on: the origin of structure in the Universe How do we make progress?How do we make progress? What are the.
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.
LIGO-G D Searching for Gravitational Waves with LIGO (Laser Interferometer Gravitational-wave Observatory) Stan Whitcomb LIGO/Caltech National.
DECIGO – Japanese Space Gravitational Wave Detector International Workshop on GPS Meteorology January 17, Tsukuba Center for Institutes Seiji Kawamura*
G R LIGO Laboratory1 The Future - How to make a next generation LIGO David Shoemaker, MIT AAAS Annual Meeting 17 February 2003.
May 23, 2002John Mather, NGST1 Adaptive Structures and Scientific Missions John Mather Senior NGST Project Scientist May 23, 2002.
The importance of Coatings for Interferometric Gravitational Wave Observatories Riccardo DeSalvo for the Coating group
Deci-hertz Interferometer Gravitational Wave Observatory (DECIGO) 7th Gravitational Wave Data Analysis Workshop December 17, International Institute.
LIGO G M Intro to LIGO Seismic Isolation Pre-bid meeting Gary Sanders LIGO/Caltech Stanford, April 29, 2003.
Space Gravitational Wave Antenna DECIGO Project 3rd TAMA Symposium February 7, Institute for Cosmic Ray Research, Japan Seiji Kawamura National.
The VIRGO detection system
Mike Cruise University of Birmingham Searching for the fifth dimension using gravitational waves.
G O D D A R D S P A C E F L I G H T C E N T E R 1 Status of LISA Jordan Camp LISA Deputy Project Scientist NASA / Goddard Space Flight Center Jan. 19,
LOGO Gravitational Waves I.S.Jang Introduction Contents ii. Waves in general relativity iii. Gravitational wave detectors.
Active Vibration Isolation using a Suspension Point Interferometer Youichi Aso Dept. Physics, University of Tokyo ASPEN Winter Conference on Gravitational.
LISA Laser Interferometer Space Antenna: The Mission Mike Cruise For the LISA Team.
Synopsis by Maria Ruiz-Gonzalez 12/8/16
Is there a future for LIGO underground?
GW related research activities in Hannover UNI/AEI
GW150914: The first direct detection of gravitational waves
Nergis Mavalvala MIT IAU214, August 2002
Workshop on Gravitational Wave Detectors, IEEE, Rome, October 21, 2004
LIGO Interferometry CLEO/QELS Joint Symposium on Gravitational Wave Detection, Baltimore, May 24, 2005 Daniel Sigg.
A. Heidmann M. Pinard J.-M. Courty P.-F. Cohadon
Presentation transcript:

G O D D A R D S P A C E F L I G H T C E N T E R 1 GW Interferometry at Goddard Space Flight Center Jordan Camp NASA / Goddard Space Flight Center Jan. 20, 2005 LIGO-G Z

G O D D A R D S P A C E F L I G H T C E N T E R 2 This Talk Frequency stabilization of lasers – Optical cavity – Molecular iodine Suspension point interferometer (SPI) for testing of low-frequency interferometry A few “politically correct” slides – New science direction for NASA

G O D D A R D S P A C E F L I G H T C E N T E R 3 Interferometry in Space Space interferometry a strategic direction in astronomy NASA and ESA are planning a significant number of space interferometry missions – SIM2010Stellar interferometry – LISA2014Gravitational Waves – TPF-C2015 TPF 2020Extra-solar terrestrial planets Darwin2020 – MAXIM2025Black Hole imager (x-rays) – Etc… Need frequency stabilized lasers for all of these…

G O D D A R D S P A C E F L I G H T C E N T E R 4 LISA – Search for Gravitational Waves A variety of astrophysical phenomena produce low- frequency gravitational waves – Massive BH binary coalescence – Massive BH capture of stellar mass BH – Galactic compact binaries LISA will measure strain from GW’s of Measure position to m, spacecraft separation of 5 x 10 9 m  / ~ for stabilized laser

G O D D A R D S P A C E F L I G H T C E N T E R 5 Methods of Laser Stabilization Frequency stabilization is only as good as the stability of the reference Optical resonator – Low-loss mirrors held fixed by ULE cavity – Length of cavity determines resonant frequency – Variable DC frequency, temperature sensitive Atomic or molecular gas transition – Gas held in transparent cell – Transition provides absolute frequency reference – Better at low frequencies, worse at high (~ 1 mHz crossover)

G O D D A R D S P A C E F L I G H T C E N T E R 6 Optical Cavities: experimental set-up Laser Isolator EOM Cavities in 5 layers of gold coated stainless steel in vacuum chamber Macor standoffs Cavities manufactured from ULE cylinders with fused silica mirrors optically contacted to end faces

G O D D A R D S P A C E F L I G H T C E N T E R 7 Results (Mueller, McNamara) ServoCrossovers LISA frequency noise requirement

G O D D A R D S P A C E F L I G H T C E N T E R 8 Thermal noise limit to cavity frequency stabilization (K. Numata) Thermal noise is fundamental limit to cavity stability Mechanical loss of spacer, mirror, coatings causes thermal noise Limit ~ 3 Hz / Hz 1/2 1 mHz Hz / Hz 1/2 100 Hz NIST and VIRGO data both limited by ULE mirror substrates (Q ~ 6 x 10 4 )

G O D D A R D S P A C E F L I G H T C E N T E R 9 Iodine laser stabilization layout Laser FI PP-MgO:LN AOM Iodine 19 MHZ EOM 21 MHZ EOM

G O D D A R D S P A C E F L I G H T C E N T E R 10 Iodine stabilization laboratory setup

G O D D A R D S P A C E F L I G H T C E N T E R 11 Iodine noise performance (20 cm length cell) V. Leonhardt Intensity Temperature Electronic Absolute frequency Insensitive to alignment and temperature

G O D D A R D S P A C E F L I G H T C E N T E R 12 Low-Frequency Interferometry Testbed Suspension Point Interferometer testing platform goal: lock platforms at picometer, nanoradian level stable platforms will allow study of interferometry, noise

G O D D A R D S P A C E F L I G H T C E N T E R 13 Suspension Point Interferometer Hexapod: 6 PZT’s for 6 DOF control  res ~ 230 Hz, Q ~ 6 2 iodine stabilized lasers: sense/control hexapod, and measure residual noise

G O D D A R D S P A C E F L I G H T C E N T E R 14 SPI Performance so far Actuator noise Sensor noise Closed loop stability Next: use ULE and bonded optics Stability limited by CTE of mechanical mounts

G O D D A R D S P A C E F L I G H T C E N T E R 15 New direction for NASA science “We support NASA’s Vision for Space Exploration….” – Moon, mars, infinity and beyond…. Science activities shifting in this direction – Earth science measurements to support planetary science of Mars, Saturn, etc. – Astrophysics must also show relevance to this (not easy…) Terrestrial planet finding now a hot subject

G O D D A R D S P A C E F L I G H T C E N T E R 16 TPF – C : Search for Terrestrial Planets Coronagraph will look for reflected light from planet by blocking direct star light from nearby stars (< 15 pc) Spectroscopy of signal will give information on composition of planetary atmosphere Water, CO 2, methane Contrast ratio of 1 : 10 9 Telescope stability is very important

G O D D A R D S P A C E F L I G H T C E N T E R 17 Interferometry in TPF-C Stabilized laser and hexapod will control secondary mirror to m, radian over hour timescale Metrology and control scheme will be developed on SPI

G O D D A R D S P A C E F L I G H T C E N T E R 18 Summary Stabilized lasers will fly! – LISA2013 – TPF-C2014 Optical resonator and molecular transition under study – Noise requirements – Space qualification SPI testbed for low-frequency space interferometry – Iodine stabilization most useful