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dc.contributor.authorStaley, A.
dc.contributor.authorMartynov, D.
dc.contributor.authorAbbott, R.
dc.contributor.authorAdhikari, R. X.
dc.contributor.authorArai, K.
dc.contributor.authorBallmer, S.
dc.contributor.authorBarsotti, Lisa
dc.contributor.authorBrooks, A. F.
dc.contributor.authorDeRosa, R. T.
dc.contributor.authorDwyer, S.
dc.contributor.authorEffler, A.
dc.contributor.authorEvans, M.
dc.contributor.authorFritschel, Peter K
dc.contributor.authorFrolov, V. V.
dc.contributor.authorGray, C.
dc.contributor.authorGuido, C. J.
dc.contributor.authorGustafson, R.
dc.contributor.authorHeintze, M.
dc.contributor.authorHoak, D.
dc.contributor.authorIzumi, K.
dc.contributor.authorKawabe, K.
dc.contributor.authorKing, E. J.
dc.contributor.authorKissel, J. S.
dc.contributor.authorKokeyama, K.
dc.contributor.authorLandry, M.
dc.contributor.authorMcClelland, D. E.
dc.contributor.authorMiller, J.
dc.contributor.authorMullavey, A.
dc.contributor.authorO'Reilly, B.
dc.contributor.authorRollins, J. G.
dc.contributor.authorSanders, J. R.
dc.contributor.authorSchofield, R. M. S.
dc.contributor.authorSigg, D.
dc.contributor.authorSlagmolen, B. J. J.
dc.contributor.authorSmith-Lefebvre, N. D.
dc.contributor.authorVajente, G.
dc.contributor.authorWard, R. L.
dc.contributor.authorWipf, Christopher C.
dc.date.accessioned2021-09-09T19:27:36Z
dc.date.available2019-06-10T16:34:55Z
dc.date.available2021-09-09T19:27:36Z
dc.date.issued2014-11
dc.date.submitted2014-09
dc.identifier.issn0264-9381
dc.identifier.issn1361-6382
dc.identifier.urihttps://hdl.handle.net/1721.1/121229.2
dc.description.abstractInterferometric gravitational-wave detectors are complex instruments comprised of a Michelson interferometer enhanced by multiple coupled cavities. Active feedback control is required to operate these instruments and keep the cavities locked on resonance. The optical response is highly nonlinear until a good operating point is reached. The linear operating range is between 0.01% and 1% of a fringe for each degree of freedom. The resonance lock has to be achieved in all five degrees of freedom simultaneously, making the acquisition difficult. Furthermore, the cavity linewidth seen by the laser is only ~1 Hz, which is four orders of magnitude smaller than the linewidth of the free running laser. The arm length stabilization system is a new technique used for arm cavity locking in Advanced LIGO. Together with a modulation technique utilizing third harmonics to lock the central Michelson interferometer, the Advanced LIGO detector has been successfully locked and brought to an operating point where detecting gravitational-waves becomes feasible.en_US
dc.publisherIOP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1088/0264-9381/31/24/245010en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourceOther repositoryen_US
dc.titleAchieving resonance in the Advanced LIGO gravitational-wave interferometeren_US
dc.typeArticleen_US
dc.identifier.citationStaley, A. et al. “Achieving Resonance in the Advanced LIGO Gravitational-Wave Interferometer.” Classical and Quantum Gravity 31, 24 (November 2014): 245010 © IOP Publishing Ltden_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physicsen_US
dc.contributor.departmentLIGO (Observatory : Massachusetts Institute of Technology)en_US
dc.contributor.departmentMIT Kavli Institute for Astrophysics and Space Researchen_US
dc.relation.journalClassical and Quantum Gravityen_US
dc.eprint.versionOriginal manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/NonPeerRevieweden_US
dc.date.updated2019-03-19T17:58:10Z
dspace.orderedauthorsStaley, A; Martynov, D; Abbott, R; Adhikari, R X; Arai, K; Ballmer, S; Barsotti, L; Brooks, A F; DeRosa, R T; Dwyer, S; Effler, A; Evans, M; Fritschel, P; Frolov, V V; Gray, C; Guido, C J; Gustafson, R; Heintze, M; Hoak, D; Izumi, K; Kawabe, K; King, E J; Kissel, J S; Kokeyama, K; Landry, M; McClelland, D E; Miller, J; Mullavey, A; OʼReilly, B; Rollins, J G; Sanders, J R; Schofield, R M S; Sigg, D; Slagmolen, B J J; Smith-Lefebvre, N D; Vajente, G; Ward, R L; Wipf, Cen_US
dspace.embargo.termsNen_US
dspace.date.submission2019-04-04T10:27:45Z
mit.journal.volume31en_US
mit.journal.issue24en_US
mit.licenseOPEN_ACCESS_POLICYen_US
mit.metadata.statusCompleteen_US


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