Relationship Between Mirrored Aperture Synthesis Radiometers and Aperture Synthesis Radiometers
The mirrored aperture synthesis radiometer (MASR) has been proposed as a new technique for high-resolution observation. Compared with ASRs, MASRs have the advantage of lower system complexity. However, the relationship between MASRs and ASRs has not been studied. In order to thoroughly study MASRs,...
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Veröffentlicht in: | IEEE geoscience and remote sensing letters 2017-05, Vol.14 (5), p.631-635 |
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description | The mirrored aperture synthesis radiometer (MASR) has been proposed as a new technique for high-resolution observation. Compared with ASRs, MASRs have the advantage of lower system complexity. However, the relationship between MASRs and ASRs has not been studied. In order to thoroughly study MASRs, it is necessary to establish the relationship between MASRs and ASRs. In this letter, the array factor of 1-D MASRs in the discrete cosine transform domain (DCT-domain) is defined. The reconstructed image for a 1-D MASR is a symmetric convolution of the observed brightness temperature distribution and the defined array factor in the DCT domain. Since a symmetric convolution can be turned into a linear convolution, the relationship between 1-D MASRs and 1-D ASRs can be established. A 1-D MASR is equivalent to a 1-D ASR that has a mirrored window. Additionally, for the equivalent 1-D ASR, its observed scene is a symmetrically extended real scene. This established relationship is validated by the simulation results. In practical applications, a MASR can be understood as an ASR. |
doi_str_mv | 10.1109/LGRS.2017.2666824 |
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Compared with ASRs, MASRs have the advantage of lower system complexity. However, the relationship between MASRs and ASRs has not been studied. In order to thoroughly study MASRs, it is necessary to establish the relationship between MASRs and ASRs. In this letter, the array factor of 1-D MASRs in the discrete cosine transform domain (DCT-domain) is defined. The reconstructed image for a 1-D MASR is a symmetric convolution of the observed brightness temperature distribution and the defined array factor in the DCT domain. Since a symmetric convolution can be turned into a linear convolution, the relationship between 1-D MASRs and 1-D ASRs can be established. A 1-D MASR is equivalent to a 1-D ASR that has a mirrored window. Additionally, for the equivalent 1-D ASR, its observed scene is a symmetrically extended real scene. This established relationship is validated by the simulation results. In practical applications, a MASR can be understood as an ASR.</description><identifier>ISSN: 1545-598X</identifier><identifier>EISSN: 1558-0571</identifier><identifier>DOI: 10.1109/LGRS.2017.2666824</identifier><identifier>CODEN: IGRSBY</identifier><language>eng</language><publisher>Piscataway: IEEE</publisher><subject>Antenna arrays ; Apertures ; Array factor ; Arrays ; Brightness temperature ; Convolution ; cosine visibility ; Discrete cosine transform ; discrete cosine transform (DCT) ; Discrete cosine transforms ; Domains ; Equivalence ; Image reconstruction ; Microwave imagery ; mirrored aperture synthesis radiometer (MASR) ; Radiometers ; Receiving antennas ; Surface radiation temperature ; symmetric convolution ; Synthesis ; Temperature distribution</subject><ispartof>IEEE geoscience and remote sensing letters, 2017-05, Vol.14 (5), p.631-635</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c293t-8273f0bfce4ca0d5c2b52eb5b61c2a51516f90f510ba02ee1d4396ab7c3525f63</citedby><cites>FETCH-LOGICAL-c293t-8273f0bfce4ca0d5c2b52eb5b61c2a51516f90f510ba02ee1d4396ab7c3525f63</cites><orcidid>0000-0002-9239-8030</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/7869341$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,792,27903,27904,54737</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/7869341$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Li, Yufang</creatorcontrib><creatorcontrib>Li, Qingxia</creatorcontrib><creatorcontrib>Feng, Li</creatorcontrib><title>Relationship Between Mirrored Aperture Synthesis Radiometers and Aperture Synthesis Radiometers</title><title>IEEE geoscience and remote sensing letters</title><addtitle>LGRS</addtitle><description>The mirrored aperture synthesis radiometer (MASR) has been proposed as a new technique for high-resolution observation. Compared with ASRs, MASRs have the advantage of lower system complexity. However, the relationship between MASRs and ASRs has not been studied. In order to thoroughly study MASRs, it is necessary to establish the relationship between MASRs and ASRs. In this letter, the array factor of 1-D MASRs in the discrete cosine transform domain (DCT-domain) is defined. The reconstructed image for a 1-D MASR is a symmetric convolution of the observed brightness temperature distribution and the defined array factor in the DCT domain. Since a symmetric convolution can be turned into a linear convolution, the relationship between 1-D MASRs and 1-D ASRs can be established. A 1-D MASR is equivalent to a 1-D ASR that has a mirrored window. Additionally, for the equivalent 1-D ASR, its observed scene is a symmetrically extended real scene. This established relationship is validated by the simulation results. In practical applications, a MASR can be understood as an ASR.</description><subject>Antenna arrays</subject><subject>Apertures</subject><subject>Array factor</subject><subject>Arrays</subject><subject>Brightness temperature</subject><subject>Convolution</subject><subject>cosine visibility</subject><subject>Discrete cosine transform</subject><subject>discrete cosine transform (DCT)</subject><subject>Discrete cosine transforms</subject><subject>Domains</subject><subject>Equivalence</subject><subject>Image reconstruction</subject><subject>Microwave imagery</subject><subject>mirrored aperture synthesis radiometer (MASR)</subject><subject>Radiometers</subject><subject>Receiving antennas</subject><subject>Surface radiation temperature</subject><subject>symmetric convolution</subject><subject>Synthesis</subject><subject>Temperature distribution</subject><issn>1545-598X</issn><issn>1558-0571</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNqFkE1Lw0AURQdRsFZ_gLgJuE6dN99Z1qJVqAipgrthkrzQlDaJM1Ok_96GFreu3l2cex8cQm6BTgBo9rCY58sJo6AnTCllmDgjI5DSpFRqOB-ykKnMzNcluQphTSkTxugRsTluXGy6NqyaPnnE-IPYJm-N953HKpn26OPOY7Lct3GFoQlJ7qqm22JEHxLX_odck4vabQLenO6YfD4_fcxe0sX7_HU2XaQly3hMDdO8pkVdoigdrWTJCsmwkIWCkjkJElSd0VoCLRxliFAJnilX6JJLJmvFx-T-uNv77nuHIdp1t_Pt4aUFkwEoyoU-UHCkSt-F4LG2vW-2zu8tUDt4tINHO3i0J4-Hzt2x0yDiH6-NyrgA_gtXNXCo</recordid><startdate>20170501</startdate><enddate>20170501</enddate><creator>Li, Yufang</creator><creator>Li, Qingxia</creator><creator>Feng, Li</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>7SP</scope><scope>7TG</scope><scope>7UA</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>FR3</scope><scope>H8D</scope><scope>H96</scope><scope>JQ2</scope><scope>KL.</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope><orcidid>https://orcid.org/0000-0002-9239-8030</orcidid></search><sort><creationdate>20170501</creationdate><title>Relationship Between Mirrored Aperture Synthesis Radiometers and Aperture Synthesis Radiometers</title><author>Li, Yufang ; Li, Qingxia ; Feng, Li</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c293t-8273f0bfce4ca0d5c2b52eb5b61c2a51516f90f510ba02ee1d4396ab7c3525f63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Antenna arrays</topic><topic>Apertures</topic><topic>Array factor</topic><topic>Arrays</topic><topic>Brightness temperature</topic><topic>Convolution</topic><topic>cosine visibility</topic><topic>Discrete cosine transform</topic><topic>discrete cosine transform (DCT)</topic><topic>Discrete cosine transforms</topic><topic>Domains</topic><topic>Equivalence</topic><topic>Image reconstruction</topic><topic>Microwave imagery</topic><topic>mirrored aperture synthesis radiometer (MASR)</topic><topic>Radiometers</topic><topic>Receiving antennas</topic><topic>Surface radiation temperature</topic><topic>symmetric convolution</topic><topic>Synthesis</topic><topic>Temperature distribution</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Yufang</creatorcontrib><creatorcontrib>Li, Qingxia</creatorcontrib><creatorcontrib>Feng, Li</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>CrossRef</collection><collection>Computer and Information Systems Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>ProQuest Computer Science Collection</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>IEEE geoscience and remote sensing letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Li, Yufang</au><au>Li, Qingxia</au><au>Feng, Li</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Relationship Between Mirrored Aperture Synthesis Radiometers and Aperture Synthesis Radiometers</atitle><jtitle>IEEE geoscience and remote sensing letters</jtitle><stitle>LGRS</stitle><date>2017-05-01</date><risdate>2017</risdate><volume>14</volume><issue>5</issue><spage>631</spage><epage>635</epage><pages>631-635</pages><issn>1545-598X</issn><eissn>1558-0571</eissn><coden>IGRSBY</coden><abstract>The mirrored aperture synthesis radiometer (MASR) has been proposed as a new technique for high-resolution observation. Compared with ASRs, MASRs have the advantage of lower system complexity. However, the relationship between MASRs and ASRs has not been studied. In order to thoroughly study MASRs, it is necessary to establish the relationship between MASRs and ASRs. In this letter, the array factor of 1-D MASRs in the discrete cosine transform domain (DCT-domain) is defined. The reconstructed image for a 1-D MASR is a symmetric convolution of the observed brightness temperature distribution and the defined array factor in the DCT domain. Since a symmetric convolution can be turned into a linear convolution, the relationship between 1-D MASRs and 1-D ASRs can be established. A 1-D MASR is equivalent to a 1-D ASR that has a mirrored window. Additionally, for the equivalent 1-D ASR, its observed scene is a symmetrically extended real scene. This established relationship is validated by the simulation results. In practical applications, a MASR can be understood as an ASR.</abstract><cop>Piscataway</cop><pub>IEEE</pub><doi>10.1109/LGRS.2017.2666824</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0002-9239-8030</orcidid></addata></record> |
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subjects | Antenna arrays Apertures Array factor Arrays Brightness temperature Convolution cosine visibility Discrete cosine transform discrete cosine transform (DCT) Discrete cosine transforms Domains Equivalence Image reconstruction Microwave imagery mirrored aperture synthesis radiometer (MASR) Radiometers Receiving antennas Surface radiation temperature symmetric convolution Synthesis Temperature distribution |
title | Relationship Between Mirrored Aperture Synthesis Radiometers and Aperture Synthesis Radiometers |
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