Single-mode waveguides for GRAVITY II. Single-mode fibers and Fiber Control Unit
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 by the telescopes are corrected with adaptive optics syste...
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creator | Perrin, G Jocou, L Perraut, K J Ph Berger Dembet, R Fédou, P Lacour, S Chapron, F Collin, C Poulain, S Cardin, V Joulain, F Eisenhauer, F Haubois, X Gillessen, S Haug, M Hausmann, F Kervella, P Léna, P Lippa, M Pfuh, O Rabien, S Amorim, A Brandner, W Straubmeier, C |
description | 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 by the telescopes are corrected with adaptive optics systems and the fringes are stabilized with a fringe-tracking system. A metrology system allows the measurement of internal path lengths in order to achieve high-accuracy astrometry. High sensitivity and high interferometric accuracy are achieved thanks to (i) correction of the turbulent phase, (ii) the use of low-noise detectors, and (iii) the optimization of photometric and coherence throughput. Beam combination and most of the beam transport are performed with single-mode waveguides in vacuum and at low temperature. In this paper, we present the functions and performance achieved with weakly birefringent standard single-mode fiber systems in GRAVITY. Fibered differential delay lines (FDDLs) are used to dynamically compensate for up to 6 mm of delay between the science and reference targets. Fibered polarization rotators allow us to align polarizations in the instrument and make the single-mode beam combiner close to polarization neutral. The single-mode fiber system exhibits very low birefringence (less than 23{\deg}), very low attenuation (3.6-7 dB/km across the K band), and optimized differential dispersion (less than 2.04 \(\mu\)rad cm2 at zero extension of the FDDLs). As a consequence, the typical fringe contrast losses due to the single-mode fibers are 6% to 10% in the lowest-resolution mode and 5% in the medium- and high-resolution modes of the instrument for a photometric throughput of the fiber chain of the order of 90%. There is no equivalent of this fiber system to route and modally filter beams with delay and polarization control in any other K-band beamcombiner. |
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Single-mode fibers and Fiber Control Unit</title><source>arXiv.org</source><source>Free E- Journals</source><creator>Perrin, G ; Jocou, L ; Perraut, K ; J Ph Berger ; Dembet, R ; Fédou, P ; Lacour, S ; Chapron, F ; Collin, C ; Poulain, S ; Cardin, V ; Joulain, F ; Eisenhauer, F ; Haubois, X ; Gillessen, S ; Haug, M ; Hausmann, F ; Kervella, P ; Léna, P ; Lippa, M ; Pfuh, O ; Rabien, S ; Amorim, A ; Brandner, W ; Straubmeier, C</creator><creatorcontrib>Perrin, G ; Jocou, L ; Perraut, K ; J Ph Berger ; Dembet, R ; Fédou, P ; Lacour, S ; Chapron, F ; Collin, C ; Poulain, S ; Cardin, V ; Joulain, F ; Eisenhauer, F ; Haubois, X ; Gillessen, S ; Haug, M ; Hausmann, F ; Kervella, P ; Léna, P ; Lippa, M ; Pfuh, O ; Rabien, S ; Amorim, A ; Brandner, W ; Straubmeier, C</creatorcontrib><description>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 by the telescopes are corrected with adaptive optics systems and the fringes are stabilized with a fringe-tracking system. A metrology system allows the measurement of internal path lengths in order to achieve high-accuracy astrometry. High sensitivity and high interferometric accuracy are achieved thanks to (i) correction of the turbulent phase, (ii) the use of low-noise detectors, and (iii) the optimization of photometric and coherence throughput. Beam combination and most of the beam transport are performed with single-mode waveguides in vacuum and at low temperature. In this paper, we present the functions and performance achieved with weakly birefringent standard single-mode fiber systems in GRAVITY. Fibered differential delay lines (FDDLs) are used to dynamically compensate for up to 6 mm of delay between the science and reference targets. Fibered polarization rotators allow us to align polarizations in the instrument and make the single-mode beam combiner close to polarization neutral. The single-mode fiber system exhibits very low birefringence (less than 23{\deg}), very low attenuation (3.6-7 dB/km across the K band), and optimized differential dispersion (less than 2.04 \(\mu\)rad cm2 at zero extension of the FDDLs). As a consequence, the typical fringe contrast losses due to the single-mode fibers are 6% to 10% in the lowest-resolution mode and 5% in the medium- and high-resolution modes of the instrument for a photometric throughput of the fiber chain of the order of 90%. There is no equivalent of this fiber system to route and modally filter beams with delay and polarization control in any other K-band beamcombiner.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2401.10613</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Adaptive optics ; Adaptive systems ; Astrometry ; Beam combiners ; Birefringence ; Control equipment ; Delay lines ; Infrared interferometers ; Low temperature ; Photometry ; Physics - Instrumentation and Methods for Astrophysics ; Polarization ; Telescopes ; Tracking systems ; Very Large Telescope ; Waveguides</subject><ispartof>arXiv.org, 2024-01</ispartof><rights>2024. This work is published under http://creativecommons.org/licenses/by-nc-nd/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://creativecommons.org/licenses/by-nc-nd/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27925</link.rule.ids><backlink>$$Uhttps://doi.org/10.1051/0004-6361/202347587$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.2401.10613$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Perrin, G</creatorcontrib><creatorcontrib>Jocou, L</creatorcontrib><creatorcontrib>Perraut, K</creatorcontrib><creatorcontrib>J Ph Berger</creatorcontrib><creatorcontrib>Dembet, R</creatorcontrib><creatorcontrib>Fédou, P</creatorcontrib><creatorcontrib>Lacour, S</creatorcontrib><creatorcontrib>Chapron, F</creatorcontrib><creatorcontrib>Collin, C</creatorcontrib><creatorcontrib>Poulain, S</creatorcontrib><creatorcontrib>Cardin, V</creatorcontrib><creatorcontrib>Joulain, F</creatorcontrib><creatorcontrib>Eisenhauer, F</creatorcontrib><creatorcontrib>Haubois, X</creatorcontrib><creatorcontrib>Gillessen, S</creatorcontrib><creatorcontrib>Haug, M</creatorcontrib><creatorcontrib>Hausmann, F</creatorcontrib><creatorcontrib>Kervella, P</creatorcontrib><creatorcontrib>Léna, P</creatorcontrib><creatorcontrib>Lippa, M</creatorcontrib><creatorcontrib>Pfuh, O</creatorcontrib><creatorcontrib>Rabien, S</creatorcontrib><creatorcontrib>Amorim, A</creatorcontrib><creatorcontrib>Brandner, W</creatorcontrib><creatorcontrib>Straubmeier, C</creatorcontrib><title>Single-mode waveguides for GRAVITY II. Single-mode fibers and Fiber Control Unit</title><title>arXiv.org</title><description>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 by the telescopes are corrected with adaptive optics systems and the fringes are stabilized with a fringe-tracking system. A metrology system allows the measurement of internal path lengths in order to achieve high-accuracy astrometry. High sensitivity and high interferometric accuracy are achieved thanks to (i) correction of the turbulent phase, (ii) the use of low-noise detectors, and (iii) the optimization of photometric and coherence throughput. Beam combination and most of the beam transport are performed with single-mode waveguides in vacuum and at low temperature. In this paper, we present the functions and performance achieved with weakly birefringent standard single-mode fiber systems in GRAVITY. Fibered differential delay lines (FDDLs) are used to dynamically compensate for up to 6 mm of delay between the science and reference targets. Fibered polarization rotators allow us to align polarizations in the instrument and make the single-mode beam combiner close to polarization neutral. The single-mode fiber system exhibits very low birefringence (less than 23{\deg}), very low attenuation (3.6-7 dB/km across the K band), and optimized differential dispersion (less than 2.04 \(\mu\)rad cm2 at zero extension of the FDDLs). As a consequence, the typical fringe contrast losses due to the single-mode fibers are 6% to 10% in the lowest-resolution mode and 5% in the medium- and high-resolution modes of the instrument for a photometric throughput of the fiber chain of the order of 90%. There is no equivalent of this fiber system to route and modally filter beams with delay and polarization control in any other K-band beamcombiner.</description><subject>Adaptive optics</subject><subject>Adaptive systems</subject><subject>Astrometry</subject><subject>Beam combiners</subject><subject>Birefringence</subject><subject>Control equipment</subject><subject>Delay lines</subject><subject>Infrared interferometers</subject><subject>Low temperature</subject><subject>Photometry</subject><subject>Physics - Instrumentation and Methods for Astrophysics</subject><subject>Polarization</subject><subject>Telescopes</subject><subject>Tracking systems</subject><subject>Very Large Telescope</subject><subject>Waveguides</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNpNj11LwzAYhYMgOOZ-gFcGvG7N-ybpx-UobhYGilbBq5Kl6cjompm2U_-93eaFV-dcPBzOQ8gNsFAkUrJ75b_tIUTBIAQWAb8gE-QcgkQgXpFZ120ZYxjFKCWfkOdX224aE-xcZeiXOpjNYCvT0dp5unyZv-fFB83zkP7Hars2vqOqrejiWGnm2t67hr61tr8ml7VqOjP7yykpFg9F9hisnpZ5Nl8FSiIGqZJSy5qZGAWAkIZJkUSoAbRgKdQxV2mkuRYxGK3ias1ZmkTj4wQqQCH5lNyeZ0-65d7bnfI_5VG7PGmPxN2Z2Hv3OZiuL7du8O34qcQUYgESEPkvVOxXXA</recordid><startdate>20240119</startdate><enddate>20240119</enddate><creator>Perrin, G</creator><creator>Jocou, L</creator><creator>Perraut, K</creator><creator>J Ph Berger</creator><creator>Dembet, R</creator><creator>Fédou, P</creator><creator>Lacour, S</creator><creator>Chapron, F</creator><creator>Collin, C</creator><creator>Poulain, S</creator><creator>Cardin, V</creator><creator>Joulain, F</creator><creator>Eisenhauer, F</creator><creator>Haubois, X</creator><creator>Gillessen, S</creator><creator>Haug, M</creator><creator>Hausmann, F</creator><creator>Kervella, P</creator><creator>Léna, P</creator><creator>Lippa, M</creator><creator>Pfuh, O</creator><creator>Rabien, S</creator><creator>Amorim, A</creator><creator>Brandner, W</creator><creator>Straubmeier, C</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20240119</creationdate><title>Single-mode waveguides for GRAVITY II. 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Single-mode fibers and Fiber Control Unit</atitle><jtitle>arXiv.org</jtitle><date>2024-01-19</date><risdate>2024</risdate><eissn>2331-8422</eissn><abstract>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 by the telescopes are corrected with adaptive optics systems and the fringes are stabilized with a fringe-tracking system. A metrology system allows the measurement of internal path lengths in order to achieve high-accuracy astrometry. High sensitivity and high interferometric accuracy are achieved thanks to (i) correction of the turbulent phase, (ii) the use of low-noise detectors, and (iii) the optimization of photometric and coherence throughput. Beam combination and most of the beam transport are performed with single-mode waveguides in vacuum and at low temperature. In this paper, we present the functions and performance achieved with weakly birefringent standard single-mode fiber systems in GRAVITY. Fibered differential delay lines (FDDLs) are used to dynamically compensate for up to 6 mm of delay between the science and reference targets. Fibered polarization rotators allow us to align polarizations in the instrument and make the single-mode beam combiner close to polarization neutral. The single-mode fiber system exhibits very low birefringence (less than 23{\deg}), very low attenuation (3.6-7 dB/km across the K band), and optimized differential dispersion (less than 2.04 \(\mu\)rad cm2 at zero extension of the FDDLs). As a consequence, the typical fringe contrast losses due to the single-mode fibers are 6% to 10% in the lowest-resolution mode and 5% in the medium- and high-resolution modes of the instrument for a photometric throughput of the fiber chain of the order of 90%. There is no equivalent of this fiber system to route and modally filter beams with delay and polarization control in any other K-band beamcombiner.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2401.10613</doi><oa>free_for_read</oa></addata></record> |
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subjects | Adaptive optics Adaptive systems Astrometry Beam combiners Birefringence Control equipment Delay lines Infrared interferometers Low temperature Photometry Physics - Instrumentation and Methods for Astrophysics Polarization Telescopes Tracking systems Very Large Telescope Waveguides |
title | Single-mode waveguides for GRAVITY II. Single-mode fibers and Fiber Control Unit |
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