DECIGO – Japanese Space Gravitational Wave Detector International Workshop on GPS Meteorology January 17, Tsukuba Center for Institutes Seiji Kawamura*

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.
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.
CLIO Current Status of Japanese Detectors Daisuke Tatsumi National Astronomical Observatory of Japan.
11-15 September Civic Auditorium TAUP2007 (Sendai) Displacement noise free interferometory for gravitational wave detection National Astronomical.
1 Science Opportunities for Australia Advanced LIGO Barry Barish Director, LIGO Canberra, Australia 16-Sept-03 LIGO-G M.
LIGO-GXX What is LIGO (LSC/GEO/Virgo/…)? Gabriela González, Louisiana State University For the LIGO Scientific Collaboration and the Virgo Collaboration.
LIGO-G W Is there a future for LIGO underground? Fred Raab, LIGO Hanford Observatory.
Status of the LIGO Project
Friday: review (HERE - A110) Monday: Final Exam 2:30 – 4:20 pm A110 (here again) Closed book, may bring 2 double- sided sheets of hand-written notes, and.
Gravitational waves LIGO (Laser Interferometer Gravitational-Wave Observatory ) in Louisiana. A laser beam is.
1 What can gravitational waves do to probe early cosmology? Barry C. Barish Caltech “Kavli-CERCA Conference on the Future of Cosmology” Case Western Reserve.
Einstein’s Theory of Gravitation “instantaneous action at a distance”
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.
Gravitational-waves: Sources and detection
The LIGO Project ( Laser Interferometer Gravitational-Wave Observatory) Rick Savage – Scientist LIGO Hanford Observatory.
LIGO -- Studying the Fabric of the Universe LIGO-GOxxxx Barry C. Barish National Science Board LIGO Livingston, LA 4-Feb-04.
What are Gravity Waves?. According to Einstein's theory of gravity, an accelerating mass causes the fabric of space-time to ripple like a pond disturbed.
Teória relativity začiatok alebo koniec fyziky.
Japanese Gravitational Wave Detectors: LCGT and DECIGO Frontiers in Optics 2009 Laser Science XXV Oct. 13, 2009 San Jose, USA Seiji Kawamura (NAOJ), LCGT.
G R 1 Ground-based GW interferometers in the LISA epoch David Shoemaker MIT LIGO 20 July 02.
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.
Paik-1 Search for Gravitational Waves Ho Jung Paik University of Maryland and Seoul National University January 12, 2006 Seoul, Korea KIAS-SNU Physics.
Optical Configuration Advanced Virgo Review Andreas Freise for the OSD subsystem.
Advanced LIGO: our future in gravitational astronomy K.A. Strain for the LIGO Science Collaboration NAM 2008 LIGO-G K.
Several Fun Research Projects at NAOJ for the Future GW Detectors
LIGO- G M Status of LIGO David Shoemaker LISA Symposium 13 July 2004.
Gravitational Wave Arezu Dehghafnar Physics Department SUT.
LIGO- G D Status of LIGO Stan Whitcomb ACIGA Workshop 21 April 2004.
The Big Bang Observer: High Laser Power for Gravitational- wave Astrophysics Gregory Harry, Peter Fritschel LIGO Laboratory, Massachusetts Institute of.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v1.
LIGO-G D “First Lock” for the LIGO Detectors 20 October 2000 LIGO Hanford Observatory Stan Whitcomb.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
1 Determination of the equation of state of the universe using 0.1Hz Gravitational Wave Antenna Takashi Nakamura and Ryuichi Takahashi Dept. Phys. Kyoto.
1 Gravitational Wave Astronomy using 0.1Hz space laser interferometer Takashi Nakamura GWDAW-8 Milwaukee 2003/12/17.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
Bridging the Gap between Terrestrial Detectors and LISA Elba 2002 May 24, 2002 Seiji Kawamura National Astronomical Observatory of Japan.
Possibility of detecting CHRISTODOULOU MEMORY of GRAVITATIONAL WAVES by using LISA (Laser Interferometer Space Antenna) Thus, the final form of the memory.
A proposal for additional Low Frequency Gravitational Wave Interferometric Detectors at LIGO Riccardo DeSalvo California Institute of Technology Globular.
Testing the slow roll inflation paradigm with the Big Bang Observer
Gravitational Waves.
LIGO-G D LIGO Laboratory1 Stoyan Nikolov LIGO-G D The LIGO project’s quest for gravitational waves Presenting LIGO to the students of.
Gravitational Wave Observatories By: Matthew Fournier.
LIGO-G D Upper Limits on the Stochastic Background of Gravitational Waves from LIGO Vuk Mandic Einstein2005 Conference Paris, July
International Gravitational Wave Network 11/9/2008 Building an Stefan Ballmer, for the LIGO / VIRGO Scientific Collaboration LIGO G
Parity violating gravitational waves Ben Owen May 21, 2009Tests of Case Western Stephon Alexander (  Haverford) Sam Finn Richard O’Shaughnessy.
LIGO-G M Scientific Operation of LIGO Gary H Sanders LIGO Laboratory California Institute of Technology APS Meeting APR03, Philadelphia Gravitational-Wave.
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.
G Z The LIGO gravitational wave detector consists of two observatories »LIGO Hanford Observatory – 2 interferometers (4 km long arms and 2 km.
LIGO-G M Press Conference Scientific Operation of LIGO Gary H Sanders Caltech (on behalf of a large team) APS April Meeting Philadelphia 6-April-03.
Space Gravitational Wave Antenna DECIGO Project 3rd TAMA Symposium February 7, Institute for Cosmic Ray Research, Japan Seiji Kawamura National.
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.
The cancelation of displacement- and frequency- noise using four mach-zehnder interferometer Keiko Kokeyama Ochanomizu University / NAOJ.
Gravitational Wave Astronomy --The Dawn has Arrived!-- 1 Misao Sasaki Yukawa Institute for Theoretical Physics Kyoto University APCTP 25 March, 2016.
LISA Laser Interferometer Space Antenna: The Mission Mike Cruise For the LISA Team.
The search for those elusive gravitational waves
Current and future ground-based gravitational-wave detectors
The Search for Gravitational Waves with Advanced LIGO
DECIGO Pathfinder Masaki Ando
Is there a future for LIGO underground?
Detection of Gravitational Waves with Interferometers
Current Status of TAMA300 Shuichi Sato
Some ideas on advanced Virgo Twins A. Giazotto-INFN Pisa
Observing Gravitational Waves(GW) by LIGO
Presentation transcript:

DECIGO – Japanese Space Gravitational Wave Detector International Workshop on GPS Meteorology January 17, Tsukuba Center for Institutes Seiji Kawamura* and DECIGO-WG (*) National Astronomical Observatory of Japan

What is Gravitational Wave? Predicted by A. Einstein in the general relativity Not yet detected directly Emitted by accelerating masses Causing a time-variant tidal strain in space Propagating with the speed of light

Detection of Gravitational Waves Using Laser Interferometer

Longer arm gives larger signals! Laser Photodetector Mirror Laser Photodetector Mirror

Large-scale GW Detectors in the World LIGO (4km) VIRGO (3km) GEO (600m) TAMA (300m) AIGO (?km) LCGT (3km)

Achievements of TAMA : World-best sensitivity obtained 2001 : World-longest 1000 hours of data obtained

Laser Interferometer in Space Signal increased - Due to longer interaction between GW and light - Cancellation of signals at higher frequencies Noise reduced - Lower seismic noise and gravity gradient noise Sensitivity improved at lower frequencies

LISA Laser Interferometer Space Antenna Joint Project by NASA and ESA Aiming at 0.1mHz - 100mHz To be launched in 2001

Gap between Terrestrial Detectors and LISA Frequency [Hz] Strain [Hz -1/2 ] LISA Terrestrial Detectors (e.g. LCGT) Gap

Importance of Bridging the Gap New window brings new science! Observe inspiral sources that have moved above the LISA band Observe inspiral sources that have not yet moved into the ground-based detector band Cosmological background could be detected Completely new sources could be detected Completely new science could be obtained

GWs from Inspirals

What is DECIGO? Deci-hertz Interferometer Gravitational Wave Observatory Space Antenna with shorter arm length Frequency [Hz] Strain [Hz -1/2 ] LISA Terrestrial Detectors (e.g. LCGT) DECIGO (Sensitivity: Arbitrary)

DECIGO Named by T. Nakamura in the PRL paper by N. Seto, S. Kawamura, and T. Nakamura Potential candidate for the future Japanese space GW antenna Study of DECIGO just started; still primitive

Relationship between Sensitivity and Arm Length Frequency [Hz] Strain [Hz -1/2 ] LISA DECIGO Shot Noise (f<f 0 ): X SN /L ∝ P -1/2 /L ∝ (L -2 ) -1/2 /L=L/L (Arm Length: x100 f0f0 f0f0 1/100 of LISA) Force Noise: x100 X FN /L ∝ 1/L f 0 :1/L f1f1 f -2

Advantages of DECIGO No confusion limiting noise above 0.1Hz (From the LISA report)

Acceleration of Expansion of the Universe NS-NS (z ~ 1) GW DECIGO Output Expansion + Acceleration? Time Strain Template (No Acceleration) Real Signal ? Phase Delay ~ 1sec (10 years) Seto, Kawamura, Nakamura, PRL 87, (2001)

Ultimate Sensitivity of DECIGO Frequency [Hz] Strain [Hz -1/2 ] LISA Terrestrial Detectors (e.g. LCGT) Ultimate DECIGO M=100kg, L=5×10 8 m) (Quantum noise limited DECIGO (LISA Technology L=5×10 7 m) Ultimate DECIGO × 1000 (Necessary for acceleration measurement)

In the Paper, we said… The ultimate sensitivity of a space antenna in the far future could be, however, 3  around 0.1 Hz in terms of strain, assuming the quantum limit sensitivity for a 100 kg mass and an arm length of 1/10 of LISA. We name this detector DECIGO. This requires an enormous amount of effective laser power, and also requires that the other noise sources, such as gravity gradient noise, thermal noise, practical noise, etc. should be all suppressed below the quantum noise. Here we assume that such an antenna may be available by the end of this century.

Necessary Technologies for DECIGO Solar Radiation Deflection of Light Gravity Gradient Three Satellite Formation Flight Drag-free Satellite Heterodyne Detection Reflection with phase- locking

How to Improve Sensitivity? Increase effective power - Increase the laser power - Increase the diameter of mirror Use shorter wavelength? Reduce other sensing noise Reduce force noise

DECIGO Working Group Convened in 2002 as one of WGs to study the future project candidates for NAOJ 1 st Meeting held on May 9, members currently involved R&D experiments to be started very soon

Two R&D Experiments to be Started Very Soon Collaboration work between NASA- Goddard (LISA) and NAOJ (DECIGO) on ground testing of space interferometry Constructing a measurement system for Earth environmental monitoring by CRL, Niigata Univ., and NAOJ

Conclusions It is important to bridge the gap between terrestrial detectors and LISA. DECIGO is a candidate for the Japanese space GW antenna. DECIGO-WG has just started investigating the possibility. R&D experiments will be started very soon.