High dynamic range imaging with a single-mode pupil remapping system: a self-calibration algorithm for redundant interferometric arrays
The correction of the influence of phase corrugation in the pupil plane is a fundamental issue in achieving high dynamic range imaging. In this paper, we investigate an instrumental set-up which consists of applying interferometric techniques on a single telescope, by filtering and dividing the pupi...
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| Published in | Monthly notices of the Royal Astronomical Society Vol. 374; no. 3; pp. 832 - 846 |
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| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
Oxford, UK
Blackwell Publishing Ltd
01.01.2007
Blackwell Science Oxford University Press Oxford University Press (OUP): Policy P - Oxford Open Option A |
| Subjects | |
| Online Access | Get full text |
| ISSN | 0035-8711 1365-8711 1365-2966 1365-2966 |
| DOI | 10.1111/j.1365-2966.2006.11198.x |
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| Summary: | The correction of the influence of phase corrugation in the pupil plane is a fundamental issue in achieving high dynamic range imaging. In this paper, we investigate an instrumental set-up which consists of applying interferometric techniques on a single telescope, by filtering and dividing the pupil with an array of single-mode fibres. We developed a new algorithm, which makes use of the fact that we have a redundant interferometric array, to completely disentangle the astronomical object from the atmospheric perturbations (phase and scintillation). This self-calibrating algorithm can also be applied to any – diluted or not – redundant interferometric set-up. On an 8-m telescope observing at a wavelength of 630 nm, our simulations show that a single-mode pupil remapping system could achieve, at a few resolution elements from the central star, a raw dynamic range up to 106, depending on the brightness of the source. The self-calibration algorithm proved to be very efficient, allowing image reconstruction of faint sources (magnitude = 15) even though the signal-to-noise ratios of individual spatial frequencies are of the order of 0.1. We finally note that the instrument could be more sensitive by combining this set-up with an adaptive optics system. The dynamic range would however be limited by the noise of the small, high-frequency displacements of the deformable mirror. |
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| Bibliography: | istex:A4B5303F4533DF7051D551CD753762DA202A60C6 ark:/67375/HXZ-P0JPFCHG-9 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 14 ObjectType-Article-1 ObjectType-Feature-2 content type line 23 |
| ISSN: | 0035-8711 1365-8711 1365-2966 1365-2966 |
| DOI: | 10.1111/j.1365-2966.2006.11198.x |