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Advanced LIGO

Authors :
Aasi, J
Abbott, B
Abbott, Robert
Abbott, T
Abernathy, M
Ackley, K
Adams, C
Adams, T
Addesso, P
Adhikari, Rana
Adya, V
Bartos, I
Charlton, Philip
Chow, Jong
Coward, D
Dhurandhar, S
Factourovich, M
Fairhurst, S
Giaime, J
Greenhalgh, R. J. S.
Hosken, Dave
Iyer, B R
Jones, D I
Mandic, V.
Mansell, Georgia
McClelland, David
Meadors, G.D.
Melatos, Andrew
Mendell, G
Nguyen, Thanh
Ottaway, D J
Owen, Benjamin
Penn, S
Rabeling, David
Rajalakshmi, G
Reed, C M
Reitze, D
Riles, K
Sammut, L
Sathyaprakash, B
Saulson, P
Schofield, R
Scott, Susan M
Shaddock, Daniel
Sigg, D
Sintes, A
Slagmolen, Bram
Souradeep, T
Staley, A
Summerscales, T.Z.
Unnikrishnan, C S
Veitch, Peter John
Vorvick, C
Wade, Andrew
Ward, Robert
Whiting, B F
Aasi, J
Abbott, B
Abbott, Robert
Abbott, T
Abernathy, M
Ackley, K
Adams, C
Adams, T
Addesso, P
Adhikari, Rana
Adya, V
Bartos, I
Charlton, Philip
Chow, Jong
Coward, D
Dhurandhar, S
Factourovich, M
Fairhurst, S
Giaime, J
Greenhalgh, R. J. S.
Hosken, Dave
Iyer, B R
Jones, D I
Mandic, V.
Mansell, Georgia
McClelland, David
Meadors, G.D.
Melatos, Andrew
Mendell, G
Nguyen, Thanh
Ottaway, D J
Owen, Benjamin
Penn, S
Rabeling, David
Rajalakshmi, G
Reed, C M
Reitze, D
Riles, K
Sammut, L
Sathyaprakash, B
Saulson, P
Schofield, R
Scott, Susan M
Shaddock, Daniel
Sigg, D
Sintes, A
Slagmolen, Bram
Souradeep, T
Staley, A
Summerscales, T.Z.
Unnikrishnan, C S
Veitch, Peter John
Vorvick, C
Wade, Andrew
Ward, Robert
Whiting, B F
Source :
Classical and Quantum Gravity
Publication Year :
2015

Abstract

The Advanced LIGO gravitational wave detectors are second-generation instruments designed and built for the two LIGO observatories in Hanford, WA and Livingston, LA, USA. The two instruments are identical in design, and are specialized versions of a Michelson interferometer with 4 km long arms. As in Initial LIGO, Fabry-Perot cavities are used in the arms to increase the interaction time with a gravitational wave, and power recycling is used to increase the effective laser power. Signal recycling has been added in Advanced LIGO to improve the frequency response. In the most sensitive frequency region around 100 Hz, the design strain sensitivity is a factor of 10 better than Initial LIGO. In addition, the low frequency end of the sensitivity band is moved from 40 Hz down to 10 Hz. All interferometer components have been replaced with improved technologies to achieve this sensitivity gain. Much better seismic isolation and test mass suspensions are responsible for the gains at lower frequencies. Higher laser power, larger test masses and improved mirror coatings lead to the improved sensitivity at mid and high frequencies. Data collecting runs with these new instruments are planned to begin in mid-2015.

Details

Database :
OAIster
Journal :
Classical and Quantum Gravity
Publication Type :
Electronic Resource
Accession number :
edsoai.on1291823768
Document Type :
Electronic Resource