Listening for Gravitational Waves 
                By: Peter Shawhan 
                  
                Gravity is part of our everyday lives, in obvious ways and in some ways  which are not so obvious.  Gravity holds the Earth together and  keeps our feet, the oceans and the atmosphere on its surface.  It  holds the gas of the Sun together in a relatively dense ball, allowing  hydrogen atoms to collide and fuse into helium, producing heat and  light.  Of course, it also keeps the Earth and other planets in  orbit around the Sun.  In daily human activities, the force of  gravity seems to be constant, but that is not quite true.  The net  gravitational pull at a given point on the Earth varies during the day  as the distances to the Sun, Moon, and other planets change; although  the variations are small, they are enough to create tides on the  oceans.  Since all  objects exert a gravitational force according to their mass, even a  truck driving by on the street outside exerts a gravitational force  while it is nearby, but (fortunately) it is much too weak to be noticed. 
                     
                  Albert Einstein, with his general theory of relativity, forged a  radical new way of thinking about gravity, in terms of "curvature" in  the geometry of space-time rather than as an ad hoc, instantaneous  force.  Among other things, the theory predicts that a  gravitational potential can bend the path of a beam of light and can  change the wavelength of the light, both of which were experimentally  confirmed in the last century.  Another prediction is that changes  in a gravitational potential propagate at the speed of light as gravitational waves, momentary  distortions of the geometry of space-time that travel outward from the  source.  Only very massive objects, changing their shape or  orientation at speeds close to the speed of light, can produce  gravitational waves with significant amplitude; but then the amplitude  falls off only as 1/r (where r is the distance from the source to the  detector), unlike the 1/r2 dependence of the gravitational  force.  Certain types of astrophysical events, such as supernova  explosions or merging black holes or neutron stars, should emit  gravitational waves that could be detected at a considerable distance,  and the waves would carry unique information about such events.   Ultimately, regular gravitational wave observations could join  electromagnetic (optical, microwave, radio, X-ray, gamma-ray) and  particle (cosmic ray, neutrino) astronomy as different ways to look at  the universe. 
                     
                  There is excellent indirect  evidence for gravitational waves from observations of orbital changes  in binary pulsar systems, but direct detection has been elusive because the wave amplitudes are incredibly  small.  A "typical" gravitational wave might produce a fractional  distortion (i.e., a strain) of only 10-21 at the Earth,  which would momentarily stretch the diameter of the Earth by about the  size of an atomic nucleus!  Joseph Weber, here at the University  of Maryland, was the first person to try to build instruments capable  of detecting such tiny signals, using suspended metal cylinders  instrumented with sensitive transducers to pick up vibrations induced  by a gravitational wave.  Weber's basic design has been improved  over the years, with major contributions made by scientists here at  Maryland, and a few such detectors are still operating.   However, physicists  are now focusing on a  
                  xnewer type of detector: a large L-shaped laser  interferometer which measures the difference  
                  xbetween the effective  lengths of the two "arms" of the L.  The Laser Interferometer   
                  xGravitational-wave Observatory (LIGO) project, funded by the National  Science Foundation, xis leading the way in this effort.  LIGO's two  observatories--in Washington State and  
                  xLouisiana--house a total of  three such detectors, with arm lengths up to 4 kilometers long. 
                  xBesides being impressive facilities when viewed from the air, they  contain cutting-edge materials and engineering: 11-kilogram cylindrical  mirrors with extremely high-quality coatings bounce laser beams back  and forth along the arms inside a vacuum enclosure, with all components  isolated from ground vibrations and other environmental disturbances as  much as possible, and held in place with sub-nanometer precision.   The arms form a sort of antenna which responds to signals coming from  most of the sky, even upward through the Earth; therefore, instead of  "looking" at a spot in the sky like an optical telescope or a radio  telescope, LIGO "listens" for gravitational waves arriving from all  around. 
                     
                  After many years of construction and commissioning, LIGO has now  reached the sensitivity it was designed for and is currently in the  middle of a long data collection run.  The data is now being  searched for many different sources, although we have limited knowledge  of what is out there--which is why this new exploration of the  gravitational-wave sky is so exciting!  For instance, we should  now be able to detect merging black holes as far away as a few hundred  million light-years, but we don't know how common black holes mergers  are in the universe.  LIGO is joined in this effort by the smaller  GEO 600 detector in Germany, and in the near future will also exchange  data with the 3-kilometer VIRGO detector in Italy in a cooperative  arrangement to analyze the data jointly for maximum sensitivity to weak  signals. 
                     
                  As a long-time member of the LIGO Scientific Collaboration (LSC), I  have helped to commission the detectors and to develop data analysis  methods and tools, and have led some of the search projects.  The  primary part of my current research plan is to search the data for  short "burst" signals of all types; it is challenging to separate a  signal from detector noise when the form of the signal is not known,  but we are refining methods for doing so.  We cannot predict when  the first gravitational-wave signal will be detected, but with patience  and care we can be ready for it when it arrives. 
                 
                Dr. Shawhan is an assistant professor of Physics for the University of Maryland . He is a member of the Gravity Experiment research group. Feel free to contact him at, pshawhan@umd.edu  .  
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