Title: Overview of LIGO
1 Overview of LIGO
Mark Coles Observatory Head LIGO Livingston
Observatory Caltech
2LIGO Laser Interferometer Gravitational-wave
Observatory
- LIGO consists of three laser interferometers
located at two sites separated by 3000 km. - The other two are at the same facility in eastern
Washington, on the Department of Energys Hanford
Nuclear Reservation, - Operated by Caltech in partnership with MIT
through a cooperative agreement with the National
Science Foundation.
3The LIGO Science Collaboration scientific body
of LIGO which defines science goals, supports
their achievement.
LSC Membership 35 institutions gt 350
collaborators
International India, Russia, Germany, U.K,
Japan and Australia.
- University of Adelaide ACIGA
- Australian National University ACIGA
- California State Dominquez Hills
- Caltech LIGO
- Caltech Experimental Gravitation CEGG
- Caltech Theory CART
- University of Cardiff GEO
- Carleton College
- Cornell University
- University of Florida _at_ Gainesville
- Glasgow University GEO
- University of Hannover GEO
- Harvard-Smithsonian
- India-IUCAA
- IAP Nizhny Novgorod
- Iowa State University
- Joint Institute of Laboratory Astrophysics
- LIGO Livingston LIGOLA
- LIGO Hanford LIGOWA
- Louisiana State University
- Louisiana Tech University
- Loyola Univ of New Orleans
- MIT LIGO
- Max Planck (Garching) GEO
- Max Planck (Potsdam) GEO
- University of Michigan
- Moscow State University
- NAOJ - TAMA
- University of Oregon
- Pennsylvania State University Exp
- Pennsylvania State University Theory
- Southern University
- Stanford University
- University of Texas_at_Brownsville
- University of Western Australia ACIGA
- University of Wisconsin_at_Milwaukee
The international partners are involved in all
aspects of the LIGO research program.
GWIC Gravitational Wave International Committee
4International network of gravitational wave
interferometers now being brought into operation
Virgo
GEO
LIGO
TAMA
Coincident detection to enhance detection
confidence source location decompose the
polarization of gravitational waves
AIGO
5LSU Participation in LIGO is broad and well
integrated
- Faculty research and student participation
- Experimentally
- Active seismic isolation
- Wave front sensors
- Interferometer characterization
- Data analysis
- Theoretically
- Quantitative descriptions of astrophysical
sources of gravity waves - Infrastructure support
- Legal support for site acquisition and permits
- liaison with state (access road)
- Internet connection and support at LSU, and with
Bell South - Outreach activities
- 16 inch LTIF telescope (with LSU Physics Prof.
Greg Guzik) - We want to encourage additional joint activities
to strengthen our partnership.
6Some History...
- Electromagnetic observation of the universe with
photons - Visible radiation
- atoms near surface of stars,
- surrounding gas clouds
- reflected radiation from planets and moons
- Other frequencies radio, x-ray, gamma ray
- Particle astrophysics
- cosmic rays
- neutrinos (solar neutrinos, SN1987 A)
- What about gravity as a messenger of
astrophysical information?
7Einsteins Theory of Gravitation gravitational
waves
- a necessary consequence of Special Relativity
with its finite speed for information transfer - Einstein in 1916 and 1918 put forward the
formulation of gravitational waves in General
Relativity - time dependent gravitational fields come from
the acceleration of masses and propagate away
from their sources as a space-time warpage at the
speed of light
gravitational radiation binary inspiral of
compact objects
8GWs from Hulse-Taylor binary
emission of gravitational waves by compact binary
system
- Only 7 kpc away
- period speeds up 14 sec from 1975-94
- orbital energy loss ?shortening of period
- deviation grows quadratically with time
- beautiful agreement (lt0.4 discrepancy) with GR
prediction of energy loss due to gravitational
radiation
9Only positive mass exists, so dipole
displacements are not allowed by conservation of
momentum
quadrupole radiation is lowest order radiation
multipole
Gravitational source from quadrupole deformation
of a sphere
10Gravitational Wave Antenna quadrupole strain
sensitivity
Displacement 10-19 meters for 4 km path!
Initial position of freely suspended test
mass Displaced test mass position
11Status
- First 16 day Science Run now in progress.
- New high water mark for gravitational wave
searches. - 9th in a series of data runs to check and
characterize the detectors, software, procedures.
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13Plans
- Further commissioning of interferometer control
systems to achieve design sensitivity - Plan to collect at least one year of integrated
coincident data during 2003-2006 - Developing plans and proposals to install a major
upgrade at both sites following data collection - Development of technologies for improved
interferometers underway - Multiple pendulum suspensions
- Active seismic isolation
- High power lasers and optics
14In an inertial reference frame Positive and
negative charge allows dipole radiation
Electromagnetic Radiation
Wave propagation direction
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