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Related papers: GRAVITY: The AO-Assisted, Two-Object Beam-Combiner…

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We present the Wavefront Sensor units of the Gravity Plus Adaptive Optics (GPAO) system, which will equip all 8m class telescopes of the VLTI and is an instrumental part of the GRAVITY+ project. It includes two modules for each Wavefront…

GRAVITY+ is the upgrade of GRAVITY and the Very Large Telescope Interferometer (VLTI) with wide-separation fringe tracking, new adaptive optics, and laser guide stars on all four 8~m Unit Telescopes (UTs), for ever fainter, all-sky, high…

Instrumentation and Methods for Astrophysics · Physics 2022-09-14 GRAVITY+ Collaboration , : , R. Abuter , F. Allouche , A. Amorim , C. Bailet , M. Bauböck , J. -P. Berger , P. Berio , A. Bigioli , O. Boebion , M. L. Bolzer , H. Bonnet , G. Bourdarot , P. Bourget , W. Brandner , Y. Clénet , B. Courtney-Barrer , Y. Dallilar , R. Davies , D. Defrère , A. Delboulbé , F. Delplancke , R. Dembet , P. T. de Zeeuw , A. Drescher , A. Eckart , C. Édouard , F. Eisenhauer , M. Fabricius , H. Feuchtgruber , G. Finger , N. M. Förster Schreiber , E. Garcia , P. Garcia , F. Gao , E. Gendron , R. Genzel , J. P. Gil , S. Gillessen , T. Gomes , F. Gonté , C. Gouvret , P. Guajardo , S. Guieu , M. Hartl , X. Haubois , F. Haußmann , G. Heißel , Th. Henning , S. Hippler , S. Hönig , M. Horrobin , N. Hubin , E. Jacqmart , L. Jochum , L. Jocou , A. Kaufer , P. Kervella , H. Korhonen , L. Kreidberg , S. Lacour , S. Lagarde , O. Lai , V. Lapeyrère , R. Laugier , J. -B. Le Bouquin , J. Leftley , P. Léna , D. Lutz , F. Mang , A. Marcotto , D. Maurel , A. Mérand , F. Millour , N. More , H. Nowacki , M. Nowak , S. Oberti , T. Ott , L. Pallanca , T. Paumard , K. Perraut , G. Perrin , R. Petrov , O. Pfuhl , N. Pourré , S. Rabien , C. Rau , S. Robbe-Dubois , S. Rochat , M. Salman , M. Schöller , J. Schubert , N. Schuhler , J. Shangguan , T. Shimizu , S. Scheithauer , A. Sevin , F. Soulez , A. Spang , E. Stadler , J. Stadler , C. Straubmeier , E. Sturm , L. J. Tacconi , K. R. W. Tristram , F. Vincent , S. von Fellenberg , S. Uysal , F. Widmann , E. Wieprecht , E. Wiezorrek , J. Woillez , S. Yazici , A. Young , G. Zins

GRAVITY is the second generation VLT Interferometer (VLTI) instrument for high-precision narrow-angle astrometry and phase-referenced interferometric imaging. The laser metrology system of GRAVITY is at the heart of its astrometric mode,…

The 2nd generation VLTI instrument GRAVITY is a two-field infrared interferometer operating in the K band between 1.97 and 2.43 $\mu$m with either the four 8 m or the four 1.8 m telescopes of the Very Large Telescope (VLT). Beams collected…

Infrared interferometry has seen a revolution over the last few years. The advent of GRAVITY+ is about to enable high-contrast observations, all-sky coverage and faint science up to K=21, with the implementation on 8m-class telescope of…

Instrumentation and Methods for Astrophysics · Physics 2024-10-30 G. Bourdarot , F. Eisenhauer

Since 2019, GRAVITY has provided direct observations of giant planets and brown dwarfs at separations of down to 95 mas from the host star. Some of these observations have provided the first direct confirmation of companions previously…

Instrumentation and Methods for Astrophysics · Physics 2024-06-07 N. Pourré , T. O. Winterhalder , J. -B. Le Bouquin , S. Lacour , A. Bidot , M. Nowak , A. -L. Maire , D. Mouillet , C. Babusiaux , J. Woillez , R. Abuter , A. Amorim , R. Asensio-Torres , W. O. Balmer , M. Benisty , J. -P. Berger , H. Beust , S. Blunt , A. Boccaletti , M. Bonnefoy , H. Bonnet , M. S. Bordoni , G. Bourdarot , W. Brandner , F. Cantalloube , P. Caselli , B. Charnay , G. Chauvin , A. Chavez , E. Choquet , V. Christiaens , Y. Clénet , V. Coudé du Foresto , A. Cridland , R. Davies , D. Defrère , R. Dembet , J. Dexter , A. Drescher , G. Duvert , A. Eckart , F. Eisenhauer , N. M. Föster Schreiber , P. Garcia , R. Garcia Lopez , E. Gendron , R. Genzel , S. Gillessen , J. H. Girard , F. Gonte , S. Grant , X. Haubois , G. Heißel , Th. Henning , S. Hinkley , S. Hippler , S. F. Hönig , M. Houllé , Z. Hubert , L. Jocou , J. Kammerer , M. Kenworthy , M. Keppler , P. Kervella , L. Kreidberg , N. T. Kurtovic , A. -M. Lagrange , V. Lapeyrère , D. Lutz , F. Mang , G. -D. Marleau , A. Mérand , F. Millour , P. Mollière , J. D. Monnier , C. Mordasini , E. Nasedkin , S. Oberti , T. Ott , G. P. L. Otten , C. Paladini , T. Paumard , K. Perraut , G. Perrin , O. Pfuhl , L. Pueyo , D. C. Ribeiro , E. Rickman , Z. Rustamkulov , J. Shangguan , T. Shimizu , D. Sing , F. Soulez , J. Stadler , T. Stolker , O. Straub , C. Straubmeier , E. Sturm , C. Sykes , L. J. Tacconi , E. F. van Dishoeck , A. Vigan , F. Vincent , S. D. von Fellenberg , J. Wang , F. Widmann , S. Yazici , the GRAVITY Collaboration , J. A. Abad , E. Aller Carpentier , J. Alonso , L. Andolfato , P. Barriga , J. -L. Beuzit , P. Bourget , R. Brast , L. Caniguante , E. Cottalorda , P. Darré , B. Delabre , A. Delboulbé , F. Delplancke-Ströbele , R. Donaldson , R. Dorn , C. Dupuy , S. Egner , G. Fischer , C. Frank , E. Fuenteseca , P. Gitton , T. Guerlet , S. Guieu , P. Gutierrez , P. Haguenauer , A. Haimerl , C. T. Heritier , S. Huber , N. Hubin , P. Jolley , J. -P. Kirchbauer , J. Kolb , J. Kosmalski , P. Krempl , M. Le Louarn , P. Lilley , B. Lopez , Y. Magnard , S. Mclay , A. Meilland , A. Meister , T. Moulin , L. Pasquini , J. Paufique , I. Percheron , L. Pettazzi , D. Phan , W. Pirani , J. Quentin , A. Rakich , R. Ridings , J. Reyes , S. Rochat , C. Schmid , N. Schuhler , P. Shchekaturov , M. Seidel , C. Soenke , E. Stadler , C. Stephan , M. Suárez , M. Todorovic , G. Valdes , C. Verinaud , G. Zins , S. Zúñiga-Fernández , the NAOMI Collaboration

A basic principle of long baseline interferometry is that an optical path difference (OPD) directly translates into an astrometric measurement. In the simplest case, the OPD is equal to the scalar product between the vector linking the two…

Instrumentation and Methods for Astrophysics · Physics 2014-09-05 S. Lacour , F. Eisenhauer , S. Gillessen , O. Pfuhl , J. Woillez , H. Bonnet , G. Perrin , B. Lazareff , S. Rabien , V. Lapeyrere , Y. Clenet , P. Kervella , Y. Kok

Context. The GRAVITY instrument on the ESO VLTI is setting a new mark in the landscape of optical interferometers. Long exposures are possible for the first time in this wavelength domain, delivering a dramatic improvement for astrophysics.…

Instrumentation and Methods for Astrophysics · Physics 2019-05-08 Guy Perrin , Julien Woillez

Two of the three instruments proposed to ESO for the second generation instrumentation of the VLTI would use integrated optics for beam combination. Several design are studied, including co-axial and multi-axial recombination. An extensive…

We present the installed and fully operational beam stabilization and fiber injection subsystem feeding the 2nd generation VLTI instrument GRAVITY. The interferometer GRAVITY requires an unprecedented stability of the VLTI optical train to…

We present simulations of Keck Interferometer ASTRA and VLTI GRAVITY observations of mock star fields in orbit within ~50 milliarcseconds of Sgr A*. Dual-field phase referencing techniques, as implemented on ASTRA and planned for GRAVITY,…

Astrophysics of Galaxies · Physics 2015-06-05 Jordan M. Stone , J. A. Eisner , J. D. Monnier , J. Woillez , P. Wizinowich , J. -U. Pott , A. M. Ghez

Infrared interferometry is a new frontier for precision ground based observing, with new instrumentation achieving milliarcsecond (mas) spatial resolutions for faint sources, along with astrometry on the order of 10 microarcseconds. This…

Our objective is to prove that integrated optics (IO) is not only a good concept for astronomical interferometry but also a working technique with high performance. We used the commissioning data obtained with the dedicated K-band…

Interferometric measurements of optical path length differences of stars over large baselines can deliver extremely accurate astrometric data. The interferometer GRAVITY will simultaneously measure two objects in the field of view of the…

With the upgrade from GRAVITY to GRAVITY$^+$ the instrument will evolve into an all-sky interferometer that can observe faint targets, such as high redshift AGN. Observing the faintest targets requires reducing the noise sources in GRAVITY…

GRAVITY acquisition camera implements four optical functions to track multiple beams of Very Large Telescope Interferometer (VLTI): a) pupil tracker: a $2 \times 2$ lenslet images four pupil reference lasers mounted on the spiders of…

Context. The GRAVITY+ upgrade implies a complete renewal of its adaptive optics (AO) systems. Its complex design, featuring moving components between the deformable mirrors and the wavefront sensors, requires the monitoring and…

We present the optical and cryo-mechanical solutions for the Spectrograph of VSI (VLTI Spectro-Imager), the second generation near-infrared (J, H and K bands) interferometric instrument for the VLTI. The peculiarity of this spectrograph is…

Astrophysics · Physics 2009-11-13 D. Lorenzetti , G. Li Causi , R. Speziali , F. Vitali , D. Loreggia , C. Baffa , P. Kern , L. Jocou , F. Malbet , P. Rabou

In the context of the GRAVITY+ upgrade, the adaptive optics (AO) systems of the GRAVITY interferometer are undergoing a major lifting. The current CILAS deformable mirrors (DM, 90 actuators) will be replaced by ALPAO kilo-DMs (43x43, 1432…