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Bringing the Visible Universe into Focus with Robo-AO
The angular resolution of ground-based optical telescopes is limited by the degrading effects of the turbulent atmosphere. In the absence of an atmosphere, the angular resolution of a typical telescope is limited only by diffraction, i.e., the wavelength of interest, λ, divided by the size of its pr...
Autores principales: | , , , , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MyJove Corporation
2013
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3622497/ https://www.ncbi.nlm.nih.gov/pubmed/23426078 http://dx.doi.org/10.3791/50021 |
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author | Baranec, Christoph Riddle, Reed Law, Nicholas M. Ramaprakash, A.N. Tendulkar, Shriharsh P. Bui, Khanh Burse, Mahesh P. Chordia, Pravin Das, Hillol K. Davis, Jack T.C. Dekany, Richard G. Kasliwal, Mansi M. Kulkarni, Shrinivas R. Morton, Timothy D. Ofek, Eran O. Punnadi, Sujit |
author_facet | Baranec, Christoph Riddle, Reed Law, Nicholas M. Ramaprakash, A.N. Tendulkar, Shriharsh P. Bui, Khanh Burse, Mahesh P. Chordia, Pravin Das, Hillol K. Davis, Jack T.C. Dekany, Richard G. Kasliwal, Mansi M. Kulkarni, Shrinivas R. Morton, Timothy D. Ofek, Eran O. Punnadi, Sujit |
author_sort | Baranec, Christoph |
collection | PubMed |
description | The angular resolution of ground-based optical telescopes is limited by the degrading effects of the turbulent atmosphere. In the absence of an atmosphere, the angular resolution of a typical telescope is limited only by diffraction, i.e., the wavelength of interest, λ, divided by the size of its primary mirror's aperture, D. For example, the Hubble Space Telescope (HST), with a 2.4-m primary mirror, has an angular resolution at visible wavelengths of ~0.04 arc seconds. The atmosphere is composed of air at slightly different temperatures, and therefore different indices of refraction, constantly mixing. Light waves are bent as they pass through the inhomogeneous atmosphere. When a telescope on the ground focuses these light waves, instantaneous images appear fragmented, changing as a function of time. As a result, long-exposure images acquired using ground-based telescopes - even telescopes with four times the diameter of HST - appear blurry and have an angular resolution of roughly 0.5 to 1.5 arc seconds at best. Astronomical adaptive-optics systems compensate for the effects of atmospheric turbulence. First, the shape of the incoming non-planar wave is determined using measurements of a nearby bright star by a wavefront sensor. Next, an element in the optical system, such as a deformable mirror, is commanded to correct the shape of the incoming light wave. Additional corrections are made at a rate sufficient to keep up with the dynamically changing atmosphere through which the telescope looks, ultimately producing diffraction-limited images. The fidelity of the wavefront sensor measurement is based upon how well the incoming light is spatially and temporally sampled(1). Finer sampling requires brighter reference objects. While the brightest stars can serve as reference objects for imaging targets from several to tens of arc seconds away in the best conditions, most interesting astronomical targets do not have sufficiently bright stars nearby. One solution is to focus a high-power laser beam in the direction of the astronomical target to create an artificial reference of known shape, also known as a 'laser guide star'. The Robo-AO laser adaptive optics system(2,3) employs a 10-W ultraviolet laser focused at a distance of 10 km to generate a laser guide star. Wavefront sensor measurements of the laser guide star drive the adaptive optics correction resulting in diffraction-limited images that have an angular resolution of ~0.1 arc seconds on a 1.5-m telescope. |
format | Online Article Text |
id | pubmed-3622497 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2013 |
publisher | MyJove Corporation |
record_format | MEDLINE/PubMed |
spelling | pubmed-36224972013-04-15 Bringing the Visible Universe into Focus with Robo-AO Baranec, Christoph Riddle, Reed Law, Nicholas M. Ramaprakash, A.N. Tendulkar, Shriharsh P. Bui, Khanh Burse, Mahesh P. Chordia, Pravin Das, Hillol K. Davis, Jack T.C. Dekany, Richard G. Kasliwal, Mansi M. Kulkarni, Shrinivas R. Morton, Timothy D. Ofek, Eran O. Punnadi, Sujit J Vis Exp Physics The angular resolution of ground-based optical telescopes is limited by the degrading effects of the turbulent atmosphere. In the absence of an atmosphere, the angular resolution of a typical telescope is limited only by diffraction, i.e., the wavelength of interest, λ, divided by the size of its primary mirror's aperture, D. For example, the Hubble Space Telescope (HST), with a 2.4-m primary mirror, has an angular resolution at visible wavelengths of ~0.04 arc seconds. The atmosphere is composed of air at slightly different temperatures, and therefore different indices of refraction, constantly mixing. Light waves are bent as they pass through the inhomogeneous atmosphere. When a telescope on the ground focuses these light waves, instantaneous images appear fragmented, changing as a function of time. As a result, long-exposure images acquired using ground-based telescopes - even telescopes with four times the diameter of HST - appear blurry and have an angular resolution of roughly 0.5 to 1.5 arc seconds at best. Astronomical adaptive-optics systems compensate for the effects of atmospheric turbulence. First, the shape of the incoming non-planar wave is determined using measurements of a nearby bright star by a wavefront sensor. Next, an element in the optical system, such as a deformable mirror, is commanded to correct the shape of the incoming light wave. Additional corrections are made at a rate sufficient to keep up with the dynamically changing atmosphere through which the telescope looks, ultimately producing diffraction-limited images. The fidelity of the wavefront sensor measurement is based upon how well the incoming light is spatially and temporally sampled(1). Finer sampling requires brighter reference objects. While the brightest stars can serve as reference objects for imaging targets from several to tens of arc seconds away in the best conditions, most interesting astronomical targets do not have sufficiently bright stars nearby. One solution is to focus a high-power laser beam in the direction of the astronomical target to create an artificial reference of known shape, also known as a 'laser guide star'. The Robo-AO laser adaptive optics system(2,3) employs a 10-W ultraviolet laser focused at a distance of 10 km to generate a laser guide star. Wavefront sensor measurements of the laser guide star drive the adaptive optics correction resulting in diffraction-limited images that have an angular resolution of ~0.1 arc seconds on a 1.5-m telescope. MyJove Corporation 2013-02-12 /pmc/articles/PMC3622497/ /pubmed/23426078 http://dx.doi.org/10.3791/50021 Text en Copyright © 2013, Journal of Visualized Experiments http://creativecommons.org/licenses/by-nc-nd/3.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution-NonCommercial-NoDerivs 3.0 Unported License. To view a copy of this license, visithttp://creativecommons.org/licenses/by-nc-nd/3.0/ |
spellingShingle | Physics Baranec, Christoph Riddle, Reed Law, Nicholas M. Ramaprakash, A.N. Tendulkar, Shriharsh P. Bui, Khanh Burse, Mahesh P. Chordia, Pravin Das, Hillol K. Davis, Jack T.C. Dekany, Richard G. Kasliwal, Mansi M. Kulkarni, Shrinivas R. Morton, Timothy D. Ofek, Eran O. Punnadi, Sujit Bringing the Visible Universe into Focus with Robo-AO |
title | Bringing the Visible Universe into Focus with Robo-AO |
title_full | Bringing the Visible Universe into Focus with Robo-AO |
title_fullStr | Bringing the Visible Universe into Focus with Robo-AO |
title_full_unstemmed | Bringing the Visible Universe into Focus with Robo-AO |
title_short | Bringing the Visible Universe into Focus with Robo-AO |
title_sort | bringing the visible universe into focus with robo-ao |
topic | Physics |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3622497/ https://www.ncbi.nlm.nih.gov/pubmed/23426078 http://dx.doi.org/10.3791/50021 |
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