Everything about Ligo totally explained
» For the Latvian holiday Ligo, see Jāņi.
LIGO stands for
Laser Interferometer Gravitational-Wave Observatory. Cofounded in 1992 by
Kip Thorne and
Ronald Drever of
Caltech and
Rainer Weiss of
MIT, LIGO is a joint project between scientists at MIT and Caltech. It is sponsored by the
National Science Foundation (NSF). At the cost of $365 million (in 2002 USD), it was the largest and most ambitious project ever funded by NSF (and still is as of 2007). The international LIGO Scientific Collaboration (LSC) is a growing group of researchers, some 600 individuals at roughly 40 institutions, working to analyze the data from LIGO and other detectors, and working toward more sensitive future detectors.
Mission
LIGO's mission is to directly observe
gravitational waves of cosmic origin. These waves were first predicted by Einstein's
Theory of General Relativity in 1916, when the technology necessary for their detection didn't yet exist. Gravitational waves were indirectly confirmed to exist when observations were made of the binary pulsar
PSR 1913+16, for which the
Nobel Prize was awarded to Hulse and Taylor in 1993.
Direct detection of gravitational waves has long been sought, for it would open up a new branch of astronomy to complement
electromagnetic telescopes and
neutrino observatories.
Joseph Weber pioneered the effort to detect gravitational waves in the
1960s through his work on
resonant mass bar detectors. Bar detectors continue to be used at six sites worldwide. By the
1970s, scientists including
Rainer Weiss realized the applicability of laser
interferometry to gravitational wave measurements.
In August 2002, LIGO began its search for cosmic gravitational waves. Emissions of gravitational waves are expected from binary systems (collisions and coalescences of
neutron stars or black holes),
supernova of massive stars (which form
neutron stars and
black holes), rotations of neutron stars with deformed crusts, and the remnants of gravitational radiation created by the birth of the universe. The observatory may in theory also observe more exotic currently hypothetical phenomena, such as gravitational waves caused by oscillating
cosmic strings or colliding
domain walls. Since the early
1990s, physicists have believed that technology is at the point where detection of gravitational waves—of significant astrophysical interest—is possible.
Observatories
LIGO operates two gravitational wave observatories in unison: the
LIGO Livingston Observatory in
Livingston, Louisiana and the
LIGO Hanford Observatory, on the
Hanford Nuclear Reservation (coordinates of central complex: ), located near
Richland, Washington. These sites are separated by 3,002 kilometers (1,876 miles). Since gravitational waves are expected to travel at the speed of light, this distance corresponds to a difference in gravitational wave arrival times of up to ten milliseconds. Through the use of
triangulation, the difference in arrival times can determine the source of the wave in the sky.
Each observatory supports an L-shaped
ultra high vacuum system, measuring 4 kilometers (2.5 miles) on each side. Up to five
interferometers can be set up in each vacuum system.
A half-length interferometer can be operated in parallel with a primary interferometer. This second detector is half the length at 2 kilometers (1.25 miles), and its
Fabry-Perot arm cavities have the same optical finesse and thus half the storage time. With half the storage time, the theoretical strain sensitivity is as good as
the full length interferometers above 200 Hz but only half as good at low frequencies.
The LIGO Livingston Observatory houses one laser
interferometer in the primary configuration. This interferometer was successfully upgraded in 2004 with an active vibration isolation system based on hydraulic actuators providing a factor of 10 isolation in the 0.1 - 5 Hz band. Seismic vibration in this band is chiefly due to
microseismic waves and anthropogenic sources (traffic, logging, etc.).
The LIGO Hanford Observatory houses one interferometer almost identical to the one at the Livingston Observatory, as well as one half-length interferometer. Hanford has been able to use its original passive seismic isolation system due to limited geologic activity in Southeastern Washington.
Operation
The primary interferometer at each site consists of mirrors suspended at each of the corners of the L; it's known as a power-recycled
Michelson interferometer with
Fabry-Perot arms. A pre-stabilized laser emits a 10 watt beam that passes through an
optical mode cleaner before reaching a beam splitter at the vertex of the L. There the beam splits into two paths, one for each arm of the L; each arm contains Fabry-Perot cavities that store the beams and increase the effective path length.
When a gravitational wave passes through the interferometer, the space-time in the local area is altered. Depending on the source of the wave and its polarization, this results in an effective change in the length of one or both of the cavities. This length change will bring the cavity very slightly out of resonance, and will cause the light currently in the cavity to become very slightly out of phase with the incoming light.
After an equivalent of approximately 75 trips down the 4 km length to the far mirrors and back again, the two separate beams leave the arms and recombine at the beam splitter. The beams returning from two arms are kept out of phase so that when the arms are both in resonance (as when there's no gravitational wave passing through), their light waves subtract, and no light should arrive at the
photodiode. When a gravitational wave passes through the interferometer, the distances along the arms of the interferometer are shortened and lengthened, causing the beams to become slightly less out of phase, so some light arrives at the photodiode, indicating a signal. Light that doesn't contain a signal is returned to the interferometer using a power recycling mirror, thus increasing the power of the light in the arms. In actual operation, noise sources can cause movement in the optics which produces similar effects to real gravitational wave signals; a great deal of the art and complexity in the instrument is in finding ways to reduce these spurious motions of the mirrors.
Observations
Based on current models of astronomical events, and the predictions of the
general theory of relativity, gravitational waves that originate tens of millions of light years from Earth are expected to distort the 4 kilometer mirror spacing by about 10
−18 m, less than one-thousandth the "diameter" of a
proton. Equivalently, this is a relative change in distance of approximately one part in 10
21. A typical event which might cause a detection event would be the late stage inspiral and merger of two 10
solar mass black holes, not necessarily located in the Milky Way galaxy, which is expected to result in a very specific sequence of signals often summarized by the slogan
chirp,
burst,
quasi-normal mode ringing,
exponential decay.
By fourth Science Run at the end of 2004, the LIGO detectors had demonstrated sensitivities in measuring these displacements to within a factor of 2 of their design.
As of
November 2005, sensitivity had reached the primary design specification of a detectable strain of one part in 10
21 over a 100 Hz bandwidth. The baseline inspiral of two roughly solar-mass neutron stars is typically expected to be observable if it occurs within about 8 million
parsecs, averaged over all directions and polarizations. In November 2005, LIGO and
GEO 600 (the German-UK interferometric detector) began a joint science run, during which they collected data for several months.
VIRGO (the French-Italian interferometric detector) joined in May 2007. The fifth science run was ended in the fall of 2007. It is hoped that after extensive analysis this may uncover perhaps two unambiguous detection events. This would be a milestone in the history of physics. In 2004, it was reported that theorists were estimating the chances of unambiguous direct detection by 2010 at one in six.
In February 2007 a short
gamma ray burst, GRB070201 which came from the direction of the
Andromeda Galaxy, failed to be observed by LIGO. This was significant as it ruled out the Andromeda Galaxy as the location of the event (provided LIGO is able to demonstrate detection of direct gravitational waves).
Future
Enhanced LIGO
Before the sixth science run is started, a series of upgrades will be executed, resulting in an improved configuration called Enhanced LIGO with two or three times the sensitivity of Initial LIGO. Some of the planned improvements are:
- Increased laser power.
- Homodyne detection.
- Output mode cleaner.
- In-vacuum readout hardware.
Enhanced LIGO will culminate in the sixth science run (S6).
Advanced LIGO
The LIGO Scientific Collaboration and international partners plan to build Advanced LIGO. This detector (formerly referred to as "LIGO 2")is designed to improve the sensitivity of Initial LIGO (LIGO 1) by more than a factor of 10. This new detector would be installed at the LIGO Observatories to replace the present detector once it has reached its goal of a year of observation, and is hoped will transform gravitational wave science into a real observational tool.
It is anticipated that this new instrument would see gravitational wave sources possibly as often as daily, with excellent signal strengths, allowing details of the waveforms to be read off and compared with theories of neutron stars, black holes, and other highly relativistic objects. The improvement of sensitivity will allow the one-year planned observation time of initial LIGO to be equaled in just several hours.
But if and when even
one verified gravitational wave event is observed by any of the worldwide detectors, it'll be a truly exciting moment for all astronomers and astrophysicists worldwide who have waited so long for such an event to be seen.
LISA
LISA, the
Laser Interferometer Space Antenna, is a proposed joint project of
NASA and the
European Space Agency to build a laser interferometer gravitational wave detector consisting of three spacecraft in solar orbit. LISA will be sensitive to gravitational waves in a different frequency band than LIGO, so the two experiments will complement each other.
Further Information
Get more info on 'Ligo'.
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