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-=======================================================================
-LIGO: Laser Interferometer Gravitational Observatory
-=======================================================================
-
-.. warning:: This is a rough work in progress!! Likely to be factual errors, poor grammar, etc.
-
-.. note:: Most of this content is based on a 2002 Caltech course taught by
- Kip Thorn [PH237]_
-
-Noise Sources
-~~~~~~~~~~~~~~~~~~~~~~
-
-For initial LIGO, seismic noise dominates below about 60Hz, suspension thermal
-noise between 60 and 180Hz, and radiation pressure shot noise above 180Hz.
-
-Sensitivity
-~~~~~~~~~~~~~~~~~~~~~
-
-Advanced LIGO will use 40kg sapphire test masses with sensitivity of about 10e-19 meters: 1/10000 of an atomic nucleus, 10e-13 of a wavelength, and half of the entire mirror's wave function.
-
-LISA
-~~~~~~~~~~~~~
-
-5e6 km separations between three spacecraft, 1 (astronomical unit, ~1.5e8 from the sun. 1 watt lasers.
-The heterodyne detection is of the beat frequencies at each spacecraft of the
-two incoming beams. Doppler shifts of spacecraft must be taken into account,
-due not only to sun radiation pressure etc, but varying gravitational fields
-from planetary orbits.
-
-The test masses inside LISA should be free falling and have relative
-separations stable to 10e-9 cm (10e-5 wavelength of light).
-
-LISA's sensitivity is in the milihertz regime.
-
-.. note: (insert LISA noise curve?)
-
-Data Analysis
-~~~~~~~~~~~~~~~~~~~~
-
-Using matched filtering (eg, take cross correlation between two waveforms,
-integrating their product), frequency sensitivity will be around the inverse
-of the number of cycles of waveform (for LIGO, around 20,000 cycles, for LISA
-around 200,000 cycles).
-
-This technique requires known, theoretically derived waveforms (within
-phase/amplitude). There are other methods when we don't have good guesses
-about the waveform we are looking for...
-