Low Frequency Observations of the Moon with the Murchison Widefield Array
A new generation of low frequency radio telescopes is seeking to observe the redshifted 21 cm signal from the Epoch of Reionization (EoR), requiring innovative methods of calibration and imaging to overcome the difficulties of widefield low frequency radio interferometry. Precise calibration will be...
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creator | McKinley, B Briggs, F Kaplan, D L Greenhill, L J Bernardi, G Bowman, J D A de Oliveira-Costa Tingay, S J Gaensler, B M Oberoi, D Johnston-Hollitt, M Arcus, W Barnes, D Bunton, J D Cappallo, R C Corey, B E Deshpande, A deSouza, L Emrich, D Goeke, R Hazelton, B J Herne, D Hewitt, J N Kasper, J C Kincaid, B B Koenig, R Kratzenberg, E Lonsdale, C J Lynch, M J McWhirter, S R Mitchell, D A Morales, M F Morgan, E Ord, S M Pathikulangara, J Prabu, T Remillard, R A Rogers, A E E Roshi, A Salah, J E Sault, R J Shankar, N Udaya Srivani, K S Stevens, J Subrahmanyan, R Wayth, R B Waterson, M Webster, R L Whitney, A R Williams, A Williams, C L Wyithe, J S B |
description | A new generation of low frequency radio telescopes is seeking to observe the redshifted 21 cm signal from the Epoch of Reionization (EoR), requiring innovative methods of calibration and imaging to overcome the difficulties of widefield low frequency radio interferometry. Precise calibration will be required to separate the small expected EoR signal from the strong foreground emission at the frequencies of interest between 80 and 300 MHz. The Moon may be useful as a calibration source for detection of the EoR signature, as it should have a smooth and predictable thermal spectrum across the frequency band of interest. Initial observations of the Moon with the Murchison Widefield Array 32 tile prototype show that the Moon does exhibit a similar trend to that expected for a cool thermally emitting body in the observed frequency range, but that the spectrum is corrupted by reflected radio emission from Earth. In particular, there is an abrupt increase in the observed flux density of the Moon within the internationally recognised Frequency Modulated (FM) radio band. The observations have implications for future low frequency surveys and EoR detection experiments that will need to take this reflected emission from the Moon into account. The results also allow us to estimate the equivalent isotropic power emitted by the Earth in the FM band and to determine how bright the Earth might appear at metre wavelengths to an observer beyond our own solar system. |
doi_str_mv | 10.48550/arxiv.1211.1433 |
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Precise calibration will be required to separate the small expected EoR signal from the strong foreground emission at the frequencies of interest between 80 and 300 MHz. The Moon may be useful as a calibration source for detection of the EoR signature, as it should have a smooth and predictable thermal spectrum across the frequency band of interest. Initial observations of the Moon with the Murchison Widefield Array 32 tile prototype show that the Moon does exhibit a similar trend to that expected for a cool thermally emitting body in the observed frequency range, but that the spectrum is corrupted by reflected radio emission from Earth. In particular, there is an abrupt increase in the observed flux density of the Moon within the internationally recognised Frequency Modulated (FM) radio band. The observations have implications for future low frequency surveys and EoR detection experiments that will need to take this reflected emission from the Moon into account. 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Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</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/10.48550/arXiv.1211.1433$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1088/0004-6256/145/1/23$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>McKinley, B</creatorcontrib><creatorcontrib>Briggs, F</creatorcontrib><creatorcontrib>Kaplan, D L</creatorcontrib><creatorcontrib>Greenhill, L J</creatorcontrib><creatorcontrib>Bernardi, G</creatorcontrib><creatorcontrib>Bowman, J D</creatorcontrib><creatorcontrib>A de Oliveira-Costa</creatorcontrib><creatorcontrib>Tingay, S J</creatorcontrib><creatorcontrib>Gaensler, B M</creatorcontrib><creatorcontrib>Oberoi, D</creatorcontrib><creatorcontrib>Johnston-Hollitt, M</creatorcontrib><creatorcontrib>Arcus, W</creatorcontrib><creatorcontrib>Barnes, D</creatorcontrib><creatorcontrib>Bunton, J D</creatorcontrib><creatorcontrib>Cappallo, R C</creatorcontrib><creatorcontrib>Corey, B E</creatorcontrib><creatorcontrib>Deshpande, A</creatorcontrib><creatorcontrib>deSouza, L</creatorcontrib><creatorcontrib>Emrich, D</creatorcontrib><creatorcontrib>Goeke, R</creatorcontrib><creatorcontrib>Hazelton, B J</creatorcontrib><creatorcontrib>Herne, D</creatorcontrib><creatorcontrib>Hewitt, J N</creatorcontrib><creatorcontrib>Kasper, J C</creatorcontrib><creatorcontrib>Kincaid, B B</creatorcontrib><creatorcontrib>Koenig, R</creatorcontrib><creatorcontrib>Kratzenberg, E</creatorcontrib><creatorcontrib>Lonsdale, C J</creatorcontrib><creatorcontrib>Lynch, M J</creatorcontrib><creatorcontrib>McWhirter, S R</creatorcontrib><creatorcontrib>Mitchell, D A</creatorcontrib><creatorcontrib>Morales, M F</creatorcontrib><creatorcontrib>Morgan, E</creatorcontrib><creatorcontrib>Ord, S M</creatorcontrib><creatorcontrib>Pathikulangara, J</creatorcontrib><creatorcontrib>Prabu, T</creatorcontrib><creatorcontrib>Remillard, R A</creatorcontrib><creatorcontrib>Rogers, A E E</creatorcontrib><creatorcontrib>Roshi, A</creatorcontrib><creatorcontrib>Salah, J E</creatorcontrib><creatorcontrib>Sault, R J</creatorcontrib><creatorcontrib>Shankar, N Udaya</creatorcontrib><creatorcontrib>Srivani, K S</creatorcontrib><creatorcontrib>Stevens, J</creatorcontrib><creatorcontrib>Subrahmanyan, R</creatorcontrib><creatorcontrib>Wayth, R B</creatorcontrib><creatorcontrib>Waterson, M</creatorcontrib><creatorcontrib>Webster, R L</creatorcontrib><creatorcontrib>Whitney, A R</creatorcontrib><creatorcontrib>Williams, A</creatorcontrib><creatorcontrib>Williams, C L</creatorcontrib><creatorcontrib>Wyithe, J S B</creatorcontrib><title>Low Frequency Observations of the Moon with the Murchison Widefield Array</title><title>arXiv.org</title><description>A new generation of low frequency radio telescopes is seeking to observe the redshifted 21 cm signal from the Epoch of Reionization (EoR), requiring innovative methods of calibration and imaging to overcome the difficulties of widefield low frequency radio interferometry. Precise calibration will be required to separate the small expected EoR signal from the strong foreground emission at the frequencies of interest between 80 and 300 MHz. The Moon may be useful as a calibration source for detection of the EoR signature, as it should have a smooth and predictable thermal spectrum across the frequency band of interest. Initial observations of the Moon with the Murchison Widefield Array 32 tile prototype show that the Moon does exhibit a similar trend to that expected for a cool thermally emitting body in the observed frequency range, but that the spectrum is corrupted by reflected radio emission from Earth. In particular, there is an abrupt increase in the observed flux density of the Moon within the internationally recognised Frequency Modulated (FM) radio band. The observations have implications for future low frequency surveys and EoR detection experiments that will need to take this reflected emission from the Moon into account. The results also allow us to estimate the equivalent isotropic power emitted by the Earth in the FM band and to determine how bright the Earth might appear at metre wavelengths to an observer beyond our own solar system.</description><subject>Calibration</subject><subject>Earth</subject><subject>Flux density</subject><subject>Frequency ranges</subject><subject>Ionization</subject><subject>Low frequencies</subject><subject>Moon</subject><subject>Physics - Cosmology and Nongalactic Astrophysics</subject><subject>Physics - Earth and Planetary Astrophysics</subject><subject>Physics - Instrumentation and Methods for Astrophysics</subject><subject>Radio emission</subject><subject>Radio telescopes</subject><subject>Solar system</subject><subject>Space 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Precise calibration will be required to separate the small expected EoR signal from the strong foreground emission at the frequencies of interest between 80 and 300 MHz. The Moon may be useful as a calibration source for detection of the EoR signature, as it should have a smooth and predictable thermal spectrum across the frequency band of interest. Initial observations of the Moon with the Murchison Widefield Array 32 tile prototype show that the Moon does exhibit a similar trend to that expected for a cool thermally emitting body in the observed frequency range, but that the spectrum is corrupted by reflected radio emission from Earth. In particular, there is an abrupt increase in the observed flux density of the Moon within the internationally recognised Frequency Modulated (FM) radio band. The observations have implications for future low frequency surveys and EoR detection experiments that will need to take this reflected emission from the Moon into account. The results also allow us to estimate the equivalent isotropic power emitted by the Earth in the FM band and to determine how bright the Earth might appear at metre wavelengths to an observer beyond our own solar system.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1211.1433</doi><oa>free_for_read</oa></addata></record> |
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subjects | Calibration Earth Flux density Frequency ranges Ionization Low frequencies Moon Physics - Cosmology and Nongalactic Astrophysics Physics - Earth and Planetary Astrophysics Physics - Instrumentation and Methods for Astrophysics Radio emission Radio telescopes Solar system Space telescopes |
title | Low Frequency Observations of the Moon with the Murchison Widefield Array |
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