{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,10,12]],"date-time":"2025-10-12T00:09:25Z","timestamp":1760227765274,"version":"build-2065373602"},"reference-count":28,"publisher":"MDPI AG","issue":"9","license":[{"start":{"date-parts":[[2022,4,29]],"date-time":"2022-04-29T00:00:00Z","timestamp":1651190400000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"funder":[{"name":"Defence Science and Technology Group"},{"name":"The University of Adelaide"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Remote Sensing"],"abstract":"<jats:p>An understanding of land and sea surface backscatter coefficients at high frequencies (HF) is required to accurately assess ionospheric propagation conditions for over-the-horizon radar. In this paper, two methods of calculating sea surface backscatter coefficients are compared. The first method is a theoretical method developed by Barrick in 1972, which treats the sea as a slightly rough surface defined by a wave height spectrum and uses a perturbation approach. The second method compares the difference between observed and modelled backscatter ionograms in which all other losses are accounted for to obtain a measurement of the sea surface backscatter coefficient. Similar trends and values for the sea surface backscatter coefficients from each method were found despite the many models and assumptions required for both these methods. However, it was noted that there was a larger range of values for the sea surface backscatter coefficients when the Barrick method was used.<\/jats:p>","DOI":"10.3390\/rs14092139","type":"journal-article","created":{"date-parts":[[2022,5,2]],"date-time":"2022-05-02T07:08:58Z","timestamp":1651475338000},"page":"2139","update-policy":"https:\/\/doi.org\/10.3390\/mdpi_crossmark_policy","source":"Crossref","is-referenced-by-count":3,"title":["A Comparison of the Barrick and Backscatter Ionogram Methods of Calculating Sea Surface Backscatter Coefficients"],"prefix":"10.3390","volume":"14","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-0376-4511","authenticated-orcid":false,"given":"Danielle","family":"Edwards","sequence":"first","affiliation":[{"name":"Defence Science and Technology Group, Edinburgh 5111, Australia"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-6011-016X","authenticated-orcid":false,"given":"Manuel","family":"Cervera","sequence":"additional","affiliation":[{"name":"Defence Science and Technology Group, Edinburgh 5111, Australia"},{"name":"School of Physical Sciences, The University of Adelaide, Adelaide 5005, Australia"}]},{"given":"Andrew","family":"MacKinnon","sequence":"additional","affiliation":[{"name":"School of Physical Sciences, The University of Adelaide, Adelaide 5005, Australia"}]}],"member":"1968","published-online":{"date-parts":[[2022,4,29]]},"reference":[{"key":"ref_1","doi-asserted-by":"crossref","first-page":"563","DOI":"10.1029\/95RS00835","article-title":"Near-grazing illumination and shadowing of rough surfaces","volume":"30","author":"Barrick","year":"1995","journal-title":"Radio Sci."},{"key":"ref_2","doi-asserted-by":"crossref","first-page":"81","DOI":"10.1016\/0011-7471(68)90029-6","article-title":"Observations of coherent backscatter of 2\u201310 MHz radio surface waves from the sea","volume":"15","author":"Crombie","year":"1968","journal-title":"Deep-Sea Res. 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