2017
DOI: 10.1117/1.oe.56.2.029701
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Distinction between image magnification and irradiance magnification: a commentary

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Cited by 2 publications
(8 citation statements)
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“…Taking L = 5.00 × 10 −03 W cm −2 sr −1 and θ = 12.9633 degrees (as indicated in figure 1(a) with up to four decimal places to retain computational accuracy), equation ( 1) yields E ≈ 7.90 × 10 −04 W cm −2 , which is the same as the axial image irradiance that is determined through nonsequential ray tracing (see figure 2). This result further highlights the observation expressed in the author's previous communication [1]. Why does equation ( 1) work for non-aplanatic lenses?…”
Section: Introductionsupporting
confidence: 86%
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“…Taking L = 5.00 × 10 −03 W cm −2 sr −1 and θ = 12.9633 degrees (as indicated in figure 1(a) with up to four decimal places to retain computational accuracy), equation ( 1) yields E ≈ 7.90 × 10 −04 W cm −2 , which is the same as the axial image irradiance that is determined through nonsequential ray tracing (see figure 2). This result further highlights the observation expressed in the author's previous communication [1]. Why does equation ( 1) work for non-aplanatic lenses?…”
Section: Introductionsupporting
confidence: 86%
“…The applicability of equation ( 1) to non-aplanatic images was also pointed out in 1966 by Gilmore [8], who had highlighted that despite texts-including even a classic book by Born and Wolf [6]-stating the assumption of aplanatism to derive equation ( 1), many practical optical systems are not aplanatic, and the axial irradiance of the images that they form seems to be given by equation (1). Gilmore applied thermodynamic arguments to show that equation ( 1) would be at least valid for the case of non-aplanatic optical imaging systems that are forming the image of extended objects.…”
Section: Introductionmentioning
confidence: 94%
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