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The search for those elusive gravitational waves

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Presentation on theme: "The search for those elusive gravitational waves"— Presentation transcript:

1 The search for those elusive gravitational waves
The LIGO detectors Precision measurement Search for the elusive waves Nergis Mavalvala (the LIGO Scientific Collaboration)

2 Understanding gravity
Newton (16th century) Universal law of gravitation Worried about action at a distance Einstein (20th century) Gravity is a warpage of space-time Matter tells spacetime how to curve  spacetime tells matter how to move

3 Gravitational waves Ripples of the space-time fabric Act like tides  for objects that are free to move, tides change lengths by fractional amounts Stretch and squeeze the space transverse to direction of propagation Emitted by non-spherical massive objects

4 Astrophysics with GWs vs. Light
Very different information, mostly mutually exclusive Difficult to predict GW sources based on EM observations Light GW Accelerating charge Accelerating mass Images Waveforms Absorbed, scattered, dispersed by matter Very small interaction; matter is transparent 100 MHz and up 10 kHz and down

5 Astrophysical sources of GW
Ingredients Lots of mass (neutron stars, black holes) Acceleration (orbits, explosions, collisions) Not spherically symmetric (not round) Colliding star corpses Coalescing binaries The big bang Earliest moments The unexpected GWs neutrinos photons now

6 Black hole mergers Contours of GWs in x polarization
Yellow contours represent tidal forces As we zoom out we see red contours of GW waves Notice that x-pol has no emission on equatorial plane. Contours of GWs in x polarization Courtesy of J. Centrella, GSFC

7 Gravitational waves -- the Evidence
Hulse & Taylor’s Binary Neutron Star System (discovered in 1973, Nobel prize in 1993) PSR Two neutron stars orbiting each other at c Compact, dense, fast  relativistic system Emit GWs and lose energy Used time of arrival of radio pulses to measure change in orbital period due to GW emission Change in orbital period NS rotates on its axis 17 times/sec. Reaches periastron (minimum separation of binary pair) every 7.75 hours. Systematic variation in arrival time of pulses. Variation in arrival time had a 7.75 hour period  binary orbit with another star. Pulsar clock slowed when traveling fastest and in strongest part of grav field (periastron). Figure shows decrease in orbital period of 76 usec/year. Shift in periastron due to decay of orbit. Y-axis = change in orbital period relative to 1975 measurement Define periastron as measure of orbital period Exactly as predicted by GR for GW emission Years

8 In our galaxy (21 thousand light years away)
Strength of GWs Hulse-Taylor binary pulsar at the end of its lifetime (100 million years from now) In our galaxy (21 thousand light years away) h ~ 10-18 In the Virgo cluster of galaxies (50 million light years away) h ~ 10-21

9 Gravitational Wave Interferometers
GW from space Effect of GW on ‘test’ masses Interferometric measurement Very small! 1000 times smaller than the nucleus of an atom

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11 Measurement and the real world
How to measure the gravitational-wave? Measure the displacements of the mirrors of the interferometer by measuring the phase shifts of the light What makes it hard? GW amplitude is small External forces also push the mirrors around Laser light has fluctuations in its phase and amplitude

12 LIGO: Laser Interferometer Gravitational-wave Observatory
3 k m ( 1 s ) MIT 4 km 2 km NSF Caltech LA 4 km

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14 Initial LIGO – Sept Initial LIGO

15 Coming soon… to an interferometer near you
Enhanced LIGO Advanced LIGO

16 Enhanced LIGO Enhanced LIGO (2008)

17 Advanced LIGO Advanced LIGO (2011)

18 An example of a GW search
Primordial Stochastic Background

19 Cosmological GW Background
10-22 sec 10+12 sec Waves now in the LIGO band were produced sec after the Big Bang WMAP 2003

20 Stochastic GW background
What’s our Universe made of? Elements in the early Universe 10-5 10-6 Dark matter 23% Initial LIGO (1 year data) Atoms 4% Speculative structures (cosmic strings) 10-8 Energy density in GWs GWs ?? 10-9 Advanced LIGO (1 year data) Sensitivity scales at sqrt(BW*T_int) for Omega, or fourth-root(BW*T_int) for strain. Dark energy 73% 10-13 Inflation

21 Global network of detectors
GEO VIRGO LIGO TAMA AIGO LIGO Detection confidence Source polarization Sky location LISA

22 Ultimate success… New Instruments, New Field, the Unexpected…

23 The End


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