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		<id>https://en.formulasearchengine.com/w/index.php?title=Natural_evolution_strategy&amp;diff=26832</id>
		<title>Natural evolution strategy</title>
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		<updated>2012-03-21T21:08:46Z</updated>

		<summary type="html">&lt;p&gt;128.122.47.32: /* Bibliography */ added link to convergence new proof&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[optics]], &#039;&#039;&#039;smear&#039;&#039;&#039; is used to refer to motion that has low temporal frequency relative to the integration/exposure time.  This typically results from a relative rate of the image with respect to the detector (e.g., caused by movement in the scene).  Smear is typically differentiated from [[jitter (optics)|jitter]], which has a higher frequency relative to the integration time.&amp;lt;ref name=EncyOptEng&amp;gt;{{Google books|rcrGlrguj1YC|Encyclopedia of optical engineering|page=2380}}&amp;lt;/ref&amp;gt;  Whereas smear refers to a relatively constant rate during the integration/exposure time, jitter refers to a relatively sinusoidal motion during the integration/exposure time.&lt;br /&gt;
&lt;br /&gt;
The equation for the optical [[Modulation transfer function]] associated with smear is the standard [[sinc]] function associated with an extended sample&lt;br /&gt;
:&amp;lt;math&amp;gt;MTF_{smear}(u) = \frac {sin(\pi \alpha u)} {\pi \alpha u}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where u is the spatial frequency and &amp;lt;math&amp;gt;\alpha&amp;lt;/math&amp;gt; is the amplitude of the smear in pixels.&amp;lt;ref&amp;gt;{{cite journal|last=Johnson|first=Jerris F.|title=Modeling imager deterministic and statistical modulation transfer functions|journal=Applied Optics|date=10 November 1993|volume=32|issue=32|pages=6503|doi=10.1364/AO.32.006503|url=http://www.opticsinfobase.org/abstract.cfm?id=40363}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Optics]]&lt;br /&gt;
[[Category:Photography]]&lt;/div&gt;</summary>
		<author><name>128.122.47.32</name></author>
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