2012
DOI: 10.1117/12.926789
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The visible tunable filtergraph for the ATST

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Cited by 26 publications
(27 citation statements)
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“…However, a significant challenge for FP design in the era of large > 4 meter class solar telescopes is the required FP aperture. As discussed by Beckers (1998), von der Lühe and Kentischer (2000), and Kentischer et al (2012), the pupil apodization effect for FPs in a telecentric mounting configuration, which from the point of view of spatial resolution is preferred over the collimated mounting, introduces velocity errors that scale with the target contrast and the beam focal ratio incident of the FPs. Typical solar requirements for velocity errors (10s of m/sec) and field-of-view (∼> 50 ) consequently require very large FPs, i.e.…”
Section: Discussionmentioning
confidence: 99%
“…However, a significant challenge for FP design in the era of large > 4 meter class solar telescopes is the required FP aperture. As discussed by Beckers (1998), von der Lühe and Kentischer (2000), and Kentischer et al (2012), the pupil apodization effect for FPs in a telecentric mounting configuration, which from the point of view of spatial resolution is preferred over the collimated mounting, introduces velocity errors that scale with the target contrast and the beam focal ratio incident of the FPs. Typical solar requirements for velocity errors (10s of m/sec) and field-of-view (∼> 50 ) consequently require very large FPs, i.e.…”
Section: Discussionmentioning
confidence: 99%
“…This type of instrument has been in use for almost two decades, e.g., the Göttingen Fabry-Pérot interferometer (Bendlin, Volkmer & Kneer 1992) and the Telecentric Etalon Solar Spectrometer (TESOS, Kentischer et al 1998) at the Vacuum Tower Telescope (VTT) on Tenerife, the Interferometric Bidimensional Spectrometer (IBIS, Cavallini 2006) at the Dunn Solar Telescope (DST) in New Mexico, and the visible-light and NIR imaging magnetographs (Denker et al 2003) Scharmer et al (2008).…”
Section: Introductionmentioning
confidence: 99%
“…At the Udaipur Solar Observatory (USO), a narrow-band imaging system (imager) has been developed using two LN etalons in tandem with an appropriate thickness ratio. Using the etalons in tandem effectively increases the free spectral range (FSR) and the spectral resolution of the system (Kentischer et al, 1998;Tritschler et al, 2002). Although inter-reflections between multi-etalons cause ghost images, these can be eliminated or minimized either by tilting the etalons with respect to each other, or by placing a prefilter in between the etalons or by both (Tritschler et al, 2002;Kleint, Feller and Gisler, 2011;Martínez Pillet et al, 2011).…”
Section: Introductionmentioning
confidence: 99%