{"id":184,"date":"2019-07-05T15:30:12","date_gmt":"2019-07-05T19:30:12","guid":{"rendered":"https:\/\/sites.bu.edu\/biomicroscopy\/?page_id=184"},"modified":"2019-07-15T09:42:54","modified_gmt":"2019-07-15T13:42:54","slug":"paw","status":"publish","type":"page","link":"https:\/\/sites.bu.edu\/biomicroscopy\/research\/paw\/","title":{"rendered":"Partitioned aperture wavefront imaging"},"content":{"rendered":"<p><img loading=\"lazy\" src=\"\/biomicroscopy\/files\/2019\/07\/PAW-principle.png\" alt=\"\" class=\"alignright wp-image-292 size-full\" width=\"344\" height=\"193\" \/>A wavefront imager provides images of the phase and amplitude of a wavefront. Several techniques for wavefront imaging have been developed. Most of these involve the use of a laser, and are thus susceptible to speckle noise. Techniques that do not require a laser generally require collimated light, meaning they are not light efficient, or require moving parts and the acquisition of multiple images, meaning they are slow. We have recently developed a wavefront imager that is fast (single shot), achromatic (works with broadband light), light efficient (works with extended sources), and simple. The technique is based on partitioning the detection aperture of a standard microscope into four quadrants with the use of four off-axis lens. These lenses provide four oblique detection images that are simultaneously acquired with a single camera. The data provided by these four images enables the reconstruction of wavefront phase and amplitude with a simple numerical algorithm that runs in real time (video rate).<\/p>\n<figure id=\"attachment55\" aria-describedby=\"caption-attachment55\" style=\"width: 368px\" class=\"wp-caption alignright\"><img loading=\"lazy\" src=\"\/biomicroscopy\/files\/2019\/06\/Surface-topography-of-4-pixels-of-a-deformable-mirror.gif\" alt=\"\" class=\"wp-image-55 size-full\" width=\"358\" height=\"274\" \/><figcaption id=\"caption-attachment55\" class=\"wp-caption-text\">17. Surface topography of 4 pixels of a deformable mirror\/ Topography calculated based on phase-gradient images acquired by a PAW microscope in reflection mode. Image acquisition was video rate. Topography precision is about 3nm.<\/figcaption><\/figure>\n<figure id=\"attachment295\" aria-describedby=\"caption-attachment295\" style=\"width: 310px\" class=\"wp-caption alignleft\"><img loading=\"lazy\" src=\"\/biomicroscopy\/files\/2019\/07\/Phase-image-of-a-cheek-cell.png\" alt=\"\" class=\"wp-image-295\" width=\"300\" height=\"299\" srcset=\"https:\/\/sites.bu.edu\/biomicroscopy\/files\/2019\/07\/Phase-image-of-a-cheek-cell.png 416w, https:\/\/sites.bu.edu\/biomicroscopy\/files\/2019\/07\/Phase-image-of-a-cheek-cell-150x150.png 150w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><figcaption id=\"caption-attachment295\" class=\"wp-caption-text\">Reconstructed phase image based on phase-gradient images acquired by trans-illumination PAW microscope.<\/figcaption><\/figure>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<ul>\n<li>R. Barankov, J.-C. Baritaux, J. Mertz, \u201cHigh-resolution 3D phase imaging using a partitioned detection aperture: a wave-optic analysis\u201d, J. Opt. Soc. Am. A. 32, 2123-2135 (2015). <a href=\"https:\/\/www.osapublishing.org\/josaa\/abstract.cfm?uri=josaa-32-11-2123\">link<\/a><\/li>\n<li>J.-C. Baritaux, C. R. Chan, J. Li, J. Mertz, \u201cView synthesis with a partitioned-aperture microscope\u201d, Opt. Lett. 39, 685-88 (2014). <a href=\"https:\/\/www.osapublishing.org\/ol\/abstract.cfm?uri=ol-39-3-685\">link<\/a><\/li>\n<li>R. Barankov and J. Mertz, \u201cSingle-exposure profilometry using partitioned aperture wavefront imaging\u201d, Opt. Lett. 38, 3961-3963 (2013). <a href=\"https:\/\/www.osapublishing.org\/ol\/abstract.cfm?uri=ol-38-19-3961\">link<\/a><\/li>\n<li>B. Parthasarathy, K. K. Chu, T. N. Ford, J. Mertz, \u201cQuantitative phase imaging using a partitioned detection aperture\u201d, Opt. Lett. 37, 4062-4064 (2012). <a href=\"https:\/\/www.osapublishing.org\/ol\/abstract.cfm?uri=ol-37-19-4062\">link<\/a><\/li>\n<li>K. K. Chu, J. Mertz, \u201cSingle exposure complementary aperture phase microscopy with polarization encoding\u201d, Opt. Lett. 37, 3798-3800 (2012). <a href=\"https:\/\/www.osapublishing.org\/ol\/abstract.cfm?uri=ol-37-18-3798\">link<\/a><\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>A wavefront imager provides images of the phase and amplitude of a wavefront. Several techniques for wavefront imaging have been developed. Most of these involve the use of a laser, and are thus susceptible to speckle noise. Techniques that do not require a laser generally require collimated light, meaning they are not light efficient, or [&hellip;]<\/p>\n","protected":false},"author":16427,"featured_media":0,"parent":98,"menu_order":23,"comment_status":"closed","ping_status":"closed","template":"page-templates\/profiles.php","meta":[],"_links":{"self":[{"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/pages\/184"}],"collection":[{"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/users\/16427"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/comments?post=184"}],"version-history":[{"count":12,"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/pages\/184\/revisions"}],"predecessor-version":[{"id":453,"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/pages\/184\/revisions\/453"}],"up":[{"embeddable":true,"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/pages\/98"}],"wp:attachment":[{"href":"https:\/\/sites.bu.edu\/biomicroscopy\/wp-json\/wp\/v2\/media?parent=184"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}