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<?xml-stylesheet type="text/xsl" media="screen" href="/~d/styles/atom10full.xsl"?><?xml-stylesheet type="text/css" media="screen" href="http://feeds.feedburner.com/~d/styles/itemcontent.css"?><feed xmlns="http://www.w3.org/2005/Atom" xmlns:openSearch="http://a9.com/-/spec/opensearch/1.1/" xmlns:georss="http://www.georss.org/georss" xmlns:gd="http://schemas.google.com/g/2005" xmlns:thr="http://purl.org/syndication/thread/1.0" xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0" gd:etag="W/&quot;DE4BQHY9fyp7ImA9WhRWFEU.&quot;"><id>tag:blogger.com,1999:blog-7700037403334000904</id><updated>2012-01-02T17:49:11.867+11:00</updated><category term="simulation" /><category term="processing" /><category term="correlators" /><category term="ARMA" /><category term="vision" /><category term="dm" /><category term="adaptive optics" /><category term="HDR" /><category term="LCD" /><category term="lasers" /><category term="benchmark" /><category term="conference" /><category term="sci-related" /><category term="biophysics" /><category term="optical" /><category term="optical storage" /><category term="encryption" /><category term="radiometry" /><category term="wfr" /><category term="analysis" /><category term="survey" /><category term="control theory" /><category term="thoughts" /><category term="mathematics" /><category term="adc" /><category term="digital" /><category term="image" /><category term="actuators" /><category term="basics" /><category term="wfs" /><category term="science" /><category term="CMOS" /><title>To Imaging, and Beyond!</title><subtitle type="html">While developing an adaptive optics simulator, I have numerous of thougths, notes and jots. I'll put them in this blog about adaptive optics, images engineering, and beyond.</subtitle><link rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml" href="http://www.mvkonnik.info/feeds/posts/default" /><link rel="alternate" type="text/html" href="http://www.mvkonnik.info/" /><link rel="next" type="application/atom+xml" href="http://www.blogger.com/feeds/7700037403334000904/posts/default?start-index=3&amp;max-results=2&amp;redirect=false&amp;orderby=published&amp;v=2" /><author><name>Mikhail Konnik</name><uri>http://www.blogger.com/profile/00835585930351720798</uri><email>noreply@blogger.com</email><gd:image rel="http://schemas.google.com/g/2005#thumbnail" width="32" height="29" src="http://4.bp.blogspot.com/_nCnVct_QOI8/SKUVOh-25AI/AAAAAAAAACI/IA41fCMBPB4/s1600-R/virens2.jpg" /></author><generator version="7.00" uri="http://www.blogger.com">Blogger</generator><openSearch:totalResults>49</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>2</openSearch:itemsPerPage><atom10:link xmlns:atom10="http://www.w3.org/2005/Atom" rel="self" type="application/atom+xml" href="http://feeds.feedburner.com/ToImagingAndBeyond" /><feedburner:info uri="toimagingandbeyond" /><atom10:link xmlns:atom10="http://www.w3.org/2005/Atom" rel="hub" href="http://pubsubhubbub.appspot.com/" /><entry gd:etag="W/&quot;D0ICQXs-eip7ImA9WhdbFEs.&quot;"><id>tag:blogger.com,1999:blog-7700037403334000904.post-1120458656236348765</id><published>2011-10-13T11:26:00.000+11:00</published><updated>2011-10-13T11:26:00.552+11:00</updated><app:edited xmlns:app="http://www.w3.org/2007/app">2011-10-13T11:26:00.552+11:00</app:edited><category scheme="http://www.blogger.com/atom/ns#" term="image" /><title>Compressed sensing: notes and remarks</title><content type="html">This short note is about the tutorial [1] on compressed sensing (CS) recently published in Optical Engineering journal. The tutorial introduces a mathematical framework that provide insight into how a high resolution image can be inferred from a relatively small number of measurements. Among other applications, such as IR imaging and compressing video sequences, astronomical applications [2] of CS are very attractive.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color: rgb(0, 0, 153);"&gt;The idea of Compressed Sensing&lt;/span&gt;&lt;br /&gt;The basic idea of CS [1] is that when the image of interest is &lt;span style="font-style: italic;"&gt;very sparse&lt;/span&gt; or highly compressible in some basis, relatively few well-chosen observations sufﬁce to reconstruct the most signiﬁcant nonzero components. It can be also considered as projecting onto incoherent measurement ensembles [2]. Such an approach  should be directly applied in the design of the detector. Devising an optical system that directly “measures” incoherent projections of the input image would provide a compression system that encodes in the analog domain.&lt;br /&gt;&lt;br /&gt;Rather than measuring each pixel and then computing a compressed representation, CS suggests that we can measure a “compressed” representation directly.&lt;br /&gt;&lt;br /&gt;The paper [1] provides a very illustrative example of searching the bright dot on a black background: instead of full comparison (N possible locations), the CS allows to do it in M=log2(N) binary measurements using binary masks.&lt;br /&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;a href="http://1.bp.blogspot.com/-oKXqArZFpRY/TokGFqV7ySI/AAAAAAAAB-U/65S1hHD90sg/s1600/CS_searching.jpg"&gt;&lt;img style="display:block; margin:0px auto 10px; text-align:center;cursor:pointer; cursor:hand;width: 400px; height: 133px;" src="http://1.bp.blogspot.com/-oKXqArZFpRY/TokGFqV7ySI/AAAAAAAAB-U/65S1hHD90sg/s400/CS_searching.jpg" alt="" id="BLOGGER_PHOTO_ID_5659061101103139106" border="0" /&gt;&lt;/a&gt;&lt;span style="font-style: italic;"&gt;The picture from the paper [1]&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;br /&gt;The key insight of CS is that, with slightly more than K well-chosen measurements, we can determine which coefficients of some basis are signiﬁcant and accurately estimate their values.&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color: rgb(0, 0, 153);"&gt;A hardware example of Compressed sensing &lt;/span&gt;&lt;br /&gt;An example of a CS imager is the rice single-pixel camera developed by Duarte et al [3,4]. This architecture &lt;span style="font-style: italic;"&gt;uses only a single detector element to image a scene&lt;/span&gt;. A digital micromirror array is used to represent a pseudorandom binary array, and the scene of interest is then projected onto that array before the aggregate intensity of the projection is measured with a single detector.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color: rgb(0, 0, 153);"&gt;Using Compressed Sensing in Astronomy&lt;/span&gt;&lt;br /&gt;Astronomical images in many ways represent a good example of highly compressible data. An example provided in [2] is Joint Recovery of Multiple Observations. In [2], they considered a case that the data are made of N=100 images such that each image is a noise-less observation of the same sky area. The goal is to propose the decompression the set of observations in a joint recovery scheme. As the paper [2] shows, CS provides better visual and quantitative results: the recover SNR for CS is 46.8 dB, while for the JPEG2000 it is only 9.77 dB.&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color: rgb(0, 0, 153);"&gt;Remarks on using the Compressed Sensing in Adaptive optics&lt;/span&gt;&lt;br /&gt;The possible application of the CS in AO can be for centroiding estimation. Indeed, the centroid image occupies only a small portion of the sensor. The multiple observations of the same centroid can lead to increased resolution in centroiding and, therefore, better overall performance of the AO system.&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color: rgb(0, 0, 153);"&gt;References:&lt;/span&gt;&lt;br /&gt;[1] Rebecca M. Willett, Roummel F. Marcia, Jonathan M. Nichols, &lt;span style="font-style: italic; font-weight: bold;"&gt;Compressed sensing for practical optical imaging systems: a tutorial&lt;/span&gt;. Optical Engineering 50(7), 072601 (July 2011).&lt;br /&gt;&lt;br /&gt;[2]  Jérôme Bobin, Jean-Luc Starck, and Roland Ottensamer, &lt;span style="font-style: italic; font-weight: bold;"&gt;Compressed Sensing in Astronomy&lt;/span&gt;, IEEE JOURNAL OF SELECTED TOPICS IN SIGNAL PROCESSING, VOL. 2, NO. 5, OCTOBER 2008.&lt;br /&gt;&lt;br /&gt;[3] M. F. Duarte, M. A. Davenport, D. Takhar, J. N. Laska, T. Sun, K.  Kelly, and R. G. Baraniuk, “&lt;span style="font-weight: bold; font-style: italic;"&gt;Single-pixel imaging via compressive sampling&lt;/span&gt;,” IEEE Signal Process. Mag. 25(2), 83–91 (2008).&lt;br /&gt;&lt;br /&gt;[4] W. L. Chan, K. Charan, D. Takhar, K. F. Kelly, R. G. Baraniuk, and D. M. Mittleman, “&lt;span style="font-style: italic; font-weight: bold;"&gt;A single-pixel terahertz imaging system based on compressed sensing&lt;/span&gt;,” Appl. Phys. Lett. 93, 121105 (2008).&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7700037403334000904-1120458656236348765?l=www.mvkonnik.info' alt='' /&gt;&lt;/div&gt;&lt;div class="feedflare"&gt;
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&lt;/div&gt;&lt;img src="http://feeds.feedburner.com/~r/ToImagingAndBeyond/~4/kJLxb0PEhI4" height="1" width="1"/&gt;</content><link rel="replies" type="application/atom+xml" href="http://www.mvkonnik.info/feeds/1120458656236348765/comments/default" title="Post Comments" /><link rel="replies" type="text/html" href="http://www.mvkonnik.info/2011/10/compressed-sensing-notes-and-remarks.html#comment-form" title="0 Comments" /><link rel="edit" type="application/atom+xml" href="http://www.blogger.com/feeds/7700037403334000904/posts/default/1120458656236348765?v=2" /><link rel="self" type="application/atom+xml" href="http://www.blogger.com/feeds/7700037403334000904/posts/default/1120458656236348765?v=2" /><link rel="alternate" type="text/html" href="http://feedproxy.google.com/~r/ToImagingAndBeyond/~3/kJLxb0PEhI4/compressed-sensing-notes-and-remarks.html" title="Compressed sensing: notes and remarks" /><author><name>virens</name><uri>http://www.blogger.com/profile/12420257446841864325</uri><email>noreply@blogger.com</email><gd:image rel="http://schemas.google.com/g/2005#thumbnail" width="32" height="29" src="http://3.bp.blogspot.com/_hM8AMxgJLzw/SKfvXQSgAEI/AAAAAAAAAx8/8TIemBrQ15w/S220/virens2.jpg" /></author><media:thumbnail xmlns:media="http://search.yahoo.com/mrss/" url="http://1.bp.blogspot.com/-oKXqArZFpRY/TokGFqV7ySI/AAAAAAAAB-U/65S1hHD90sg/s72-c/CS_searching.jpg" height="72" width="72" /><thr:total>0</thr:total><feedburner:origLink>http://www.mvkonnik.info/2011/10/compressed-sensing-notes-and-remarks.html</feedburner:origLink></entry><entry gd:etag="W/&quot;DkEEQXY9eyp7ImA9WhdVGU4.&quot;"><id>tag:blogger.com,1999:blog-7700037403334000904.post-1818552718261270130</id><published>2011-09-25T17:10:00.000+10:00</published><updated>2011-09-25T17:10:00.863+10:00</updated><app:edited xmlns:app="http://www.w3.org/2007/app">2011-09-25T17:10:00.863+10:00</app:edited><category scheme="http://www.blogger.com/atom/ns#" term="conference" /><title>SPIE Optical Engineering and Applications 2011 - presentations from Astromentry section</title><content type="html">Some interesting papers from the Astrometry section that held on Wednesday. This is not about the Adaptive optics, but still contains some interesting points.&lt;br /&gt;
&lt;br /&gt;
&lt;a name='more'&gt;&lt;/a&gt;&lt;br /&gt;&lt;b style="color: #073763;"&gt;&amp;nbsp;&lt;/b&gt;&lt;br /&gt;
&lt;div style="color: #073763;"&gt;
&lt;b&gt;1. Differention Tip-Tilt Jitter.&lt;/b&gt;&lt;/div&gt;
&lt;div class="separator" style="clear: both; text-align: center;"&gt;
&lt;a href="http://2.bp.blogspot.com/-fewIcEXXzpo/Tl8uFYqFZ2I/AAAAAAAAB9E/SQMjIgUmgvQ/s1600/tt_jitter_01.jpg" imageanchor="1" style="margin-left: 1em; margin-right: 1em;"&gt;&lt;img border="0" height="240" src="http://2.bp.blogspot.com/-fewIcEXXzpo/Tl8uFYqFZ2I/AAAAAAAAB9E/SQMjIgUmgvQ/s320/tt_jitter_01.jpg" width="320" /&gt;&lt;/a&gt;&lt;/div&gt;
&lt;br /&gt;
It is well known fact that the Tip/Tilt is the main source of distrubance in atmospherical seeing. Other distortions to consider are geometrical ones, like cushion/barrel.&lt;br /&gt;
&lt;div class="separator" style="clear: both; text-align: center;"&gt;
&lt;a href="http://1.bp.blogspot.com/-H7u5U_HaDnQ/Tl8u-PWQTBI/AAAAAAAAB9I/6LLeoelH8WM/s1600/tt_jitter_02.jpg" imageanchor="1" style="margin-left: 1em; margin-right: 1em;"&gt;&lt;img border="0" height="253" src="http://1.bp.blogspot.com/-H7u5U_HaDnQ/Tl8u-PWQTBI/AAAAAAAAB9I/6LLeoelH8WM/s320/tt_jitter_02.jpg" width="320" /&gt;&lt;/a&gt;&lt;/div&gt;
&lt;br /&gt;
Atmosphere is like a prism - it can displace the star position. Advantages of large telescopes are therefore reduced by CDAR noise. &lt;br /&gt;
&lt;br /&gt;
&lt;div style="color: #073763;"&gt;
&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;
&lt;div style="color: #073763;"&gt;
&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;
&lt;b&gt;&lt;span style="color: #073763;"&gt;Dynamic distortion calibration using a diffracting pupil: high-precision astrometry laboratory demonstration for exoplanet detection,&lt;/span&gt;&lt;span style="color: #073763;"&gt; . . . . . . [8151-29]&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;
&lt;div class="separator" style="clear: both; text-align: center;"&gt;
&lt;a href="http://4.bp.blogspot.com/-o9jqPB7mEw4/Tl8vztSihwI/AAAAAAAAB9M/5DOOl3ReW98/s1600/exo_01.jpg" imageanchor="1" style="margin-left: 1em; margin-right: 1em;"&gt;&lt;img border="0" height="273" src="http://4.bp.blogspot.com/-o9jqPB7mEw4/Tl8vztSihwI/AAAAAAAAB9M/5DOOl3ReW98/s320/exo_01.jpg" width="320" /&gt;&lt;/a&gt;&lt;/div&gt;
&lt;br /&gt;
&lt;br /&gt;
They want to create diffraction spikes.&amp;nbsp; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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