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| 001 | 9.875695 |
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| 003 | CaOODSP |
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| 005 | 20240221113057 |
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| 006 | m o d f |
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| 007 | cr ||||||||||| |
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| 008 | 190628t20182018quca fobt f000 0 eng d |
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| 040 | |aCaOODSP|beng|erda|cCaOODSP |
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| 043 | |an-cn--- |
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| 086 | 1 |aD68-11/007-2018E-PDF |
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| 100 | 1 |aPotvin, G., |eauthor. |
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| 245 | 10|aActive turbulent imaging simulation on weak specular targets / |cGuy Potvin. |
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| 264 | 1|aQuebec (Quebec) : |bDRDC, Valcartier Research Centre, |cFebruary 2018. |
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| 264 | 4|c©2018 |
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| 300 | |a1 online resource (7 pages, 2 unnumbered pages) : |billustrations (mostly black and white). |
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| 336 | |atext|btxt|2rdacontent |
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| 337 | |acomputer|bc|2rdamedia |
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| 338 | |aonline resource|bcr|2rdacarrier |
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| 490 | 1 |aExternal Literature (N) ; |vDRDC-RDDC-2018-N007 |
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| 500 | |aTitle from cover. |
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| 500 | |a"Can unclassified." |
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| 500 | |a"February 2018." |
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| 500 | |a"Date of Publication from Ext Publisher: February 2018." |
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| 500 | |aOriginally produced for : 8th International Symposium on Optronics In Defence and Security, OPTRO2018, 6–8 February 2018, Paris, France. |
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| 504 | |aIncludes bibliographical references (page 7). |
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| 520 | 3 |a"We define the Bidirectional Reflectivity Distribution Function (BRDF) in terms of Wigner functions so as to make its radiometric aspect compatible with the wave aspect of coherent propagation through atmospheric turbulence. We then adapt this definition in order to make it compatible with the DRDC turbulent imaging simulator for active imaging on weakly specular surfaces. This is done by defining a coherence length associated with the surface which expresses how specular it is. We demonstrate our model on a few targets and comment on its range of applicability"--Abstract, p. 1. |
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| 693 | 4|aImaging simulation |
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| 710 | 1 |aDefence R&D Canada. |bValcartier Research Centre. |
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| 830 | #0|aExternal literature (N) (Defence R&D Canada)|vDRDC-RDDC-2018-N007.|w(CaOODSP)9.858173 |
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| 856 | 40|qPDF|s944 KB|uhttps://publications.gc.ca/collections/collection_2019/rddc-drdc/D68-11-007-2018-eng.pdf |
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