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dc.contributor.authorGonzález, J. J.
dc.contributor.authorCepa, J.
dc.contributor.authorGonzález Serrano, José Ignacio 
dc.contributor.authorSánchez-Portal, M.
dc.contributor.otherUniversidad de Cantabriaes_ES
dc.date.accessioned2022-06-30T13:44:28Z
dc.date.available2022-06-30T13:44:28Z
dc.date.issued2014-10
dc.identifier.issn0035-8711
dc.identifier.issn1365-2966
dc.identifier.otherAYA2011-29517-C03-01es_I
dc.identifier.otherAYA2011-29517-C03-02es_ES
dc.identifier.otherCSD2006-00070es_ES
dc.identifier.urihttp://hdl.handle.net/10902/25229
dc.description.abstractTunable filters (TFs) are a powerful way of implementing narrow-band imaging mode over wide wavelength ranges, without the need of purchasing a large number of narrow-band filters covering all strong emission or absorption lines at any redshift. However, one of its main features is a wavelength variation across the field of view, sometimes termed the phase effect. In this work, an anomalous phase effect is reported and characterized for the Optical System for Imaging and low Resolution Integrated Spectroscopy (OSIRIS) instrument at the 10.4 m Gran Telescopio Canarias. The transmitted wavelength across the field of view of the instrument depends, not only on the distance to the optical centre, but on wavelength. This effect is calibrated for the red TF of OSIRIS by measuring both normal-incidence light at laboratory and spectral lamps at the telescope at non-normal incidence. This effect can be explained by taking into account the inner coatings of the etalon. In a high spectral resolution etalon, the gap between plates is much larger than the thickness of the inner reflective coatings. In the case of a TF, like that in OSIRIS, the coatings thickness could be of the order of the cavity, which changes drastically the effective gap of the etalon. We show that by including thick and dispersive coatings into the interference equations, the observed anomalous phase effect can be perfectly reproduced. In fact, we find that, for the OSIRIS red TF, a two-coatings model fits the data with an rms of 0.5 Å at all wavelengths and incidence angles. This is a general physical model that can be applied to other TF instruments.es_ES
dc.description.sponsorshipThis work has been partially funded by the Spanish Ministry of Science and Innovation (MICINN) under the Consolider-Ingenio 2010 Programme grant CSD2006-00070: First Science with the GTC (http://www.iac.es/consolider-ingenio-gtc), AYA2011-29517-C03-01, and AYA2011-29517-C03-02. Observations presented in this paper were made with the Gran Telescopio Canarias (GTC), installed in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofsica de Canarias, on the island of La Palma.es_ES
dc.format.extent13 p.es_ES
dc.language.isoenges_ES
dc.publisherOxford University Presses_ES
dc.rights© 2014 The Authorses_ES
dc.sourceMonthly Notices of the Royal Astronomical Society, 2014, 443(4), 3289-3301es_ES
dc.subject.otherInstrumentation: interferometerses_ES
dc.subject.otherInstrumentation: spectrographses_ES
dc.titleGeneral formulation for the calibration and characterization of narrow-gap etalons: the OSIRIS/GTC tunable filters casees_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publisherVersionhttps://doi.org/10.1093/mnras/stu1310es_ES
dc.rights.accessRightsopenAccesses_ES
dc.identifier.DOI10.1093/mnras/stu1310
dc.type.versionpublishedVersiones_ES


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