{"id":61368,"date":"2016-07-19T15:12:00","date_gmt":"2016-07-19T19:12:00","guid":{"rendered":"https:\/\/www.nasa.gov\/?migration=converted-node-386652"},"modified":"2023-07-26T15:12:59","modified_gmt":"2023-07-26T19:12:59","slug":"four-mirror-freeform-reflective-imaging-systems","status":"publish","type":"post","link":"https:\/\/www.nasa.gov\/directorates\/stmd\/space-tech-research-grants\/four-mirror-freeform-reflective-imaging-systems\/","title":{"rendered":"Four-Mirror Freeform Reflective Imaging Systems"},"content":{"rendered":"\n<p><strong>Jonathan Papa<\/strong><br>\n<em>University of Rochester<\/em><\/p>\n\n\n<div id=\"\" class=\"hds-media hds-module wp-block-image\"><div class=\"margin-left-auto margin-right-auto nasa-block-align-inline\"><div class=\"hds-media-wrapper margin-left-auto margin-right-auto\"><figure class=\"hds-media-inner hds-cover-wrapper hds-media-ratio-none \"><a href=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg\"><img fetchpriority=\"high\" decoding=\"async\" width=\"1640\" height=\"2048\" src=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?w=1640\" class=\"attachment-2048x2048 size-2048x2048\" alt=\"Jonathan Papa\" style=\"transform: scale(1); transform-origin: 50% 50%; object-position: 50% 50%; object-fit: cover;\" block_context=\"nasa-block\" srcset=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg 1932w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=240,300 240w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=768,959 768w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=820,1024 820w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=1230,1536 1230w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=1640,2048 1640w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=320,400 320w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=481,600 481w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=721,900 721w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=961,1200 961w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?resize=1602,2000 1602w\" sizes=\"(max-width: 1640px) 100vw, 1640px\" loading=\"eager\" \/><\/a><\/figure><figcaption class=\"hds-caption padding-y-2\"><div class=\"hds-caption-text p-sm margin-0\">Jonathan Papa<\/div><\/figcaption><\/div><\/div><\/div>\n\n\n<p>Central Objectives: The research involves a revelation of the solution space for revolutionary families of four-mirror freeform reflective imaging systems. A freeform optical system is one that lacks rotational symmetry, meaning there is no constraint on the surface shape of the mirrors. Freeform designs can mitigate the disadvantages that prevent reflective systems from being used in larger field of view applications by yielding unobscured designs and leveraging the added freedom of surface shape to better correct the optical aberrations in the system. Freeform designs are made unobscured by breaking the axis of rotational-symmetry and tilting the individual elements themselves. They do not require an offset aperture or field bias, which brings a unique advantage in the correction of optical aberrations. By getting the mirrors out of their own way, more surfaces can be introduced. When compared to alternate solutions, whether it is a rotationally symmetric system or an unobscured system with the same number of elements, an increased diffraction-limited field of view has been demonstrated in our group\u2019s research.<\/p>\n\n\n\n<p>Methods\/Techniques: The exploration of the solution space will be accomplished by expanding upon the work of Andrew Rakich, who derived the analytical solution space for four-mirror anastigmat telescopes. The systems that are yielded from his method have spherical surfaces and an axis of rotational symmetry. These designs will be used as starting points for subsequent freeform designs. Lens design software will be used to optimize the design as the elements are tilted. When tilting elements, very strong astigmatism is introduced. Therefore, toroidal base mirrors for the freeform surfaces are needed for correction. Zernike polynomials are then introduced to the toroidal base shapes to further correct the system. The research aims to explore a variety of targeted research questions that aim to address space technology challenges. The sensitivity of the designs from the solution space to common tolerances will be studied using full-field displays that isolate each aberration and show its dependence over the field, combined with Nodal Aberration Theory that puts tolerances in linear space, making the sensitivity calculation efficient and complete. Special attention will be paid to geometries that may be more conducive to stray light reduction through the use of baffles. Similarly, other geometries may be more conducive to radiation shielding by using the mirror substrates themselves as part of the shielding. The added flexibility of folding geometry allows for the design to be tailored to system engineering constraints that could not be addressed with rotationally symmetric systems or unobscured non-freeform systems. Design approaches to achieve these characteristics will be developed.<\/p>\n\n\n\n<p>Significance: This research will address NASA interests as per the July 2015 technology roadmap item TA 8.2.1.3. A key, driving aspect of this work will be to focus on revealing key flat field Large, low cost, lightweight precision monolithic mirrors that provide a high degree of thermal and dynamic stability, and wavefront sensing and control for Ultra-Stable Large-Aperture UV\/Visible\/Near-IR telescopes. \u009d This research is directly relevant to the Observatories \u009d level 2 TABS element, 8.2. More specifically, it is relevant to the level 3 TABS element Mirror Systems. \u009d The significance of this work is to provide imaging system designs with larger diffraction-limited etendues than the state-of-the-art, (meaning larger apertures and fields of view), which will make the most of limited package sizes and mass constraints. This will advance the optical instrumentation on space probes as well as observatories on the ground towards new space discoveries and knowledge.<\/p>\n\n\n\n<p><a href=\"\/directorates\/spacetech\/strg\/nstrf-2016\"><strong>Back to NSTRF 2016 Full List<\/strong><\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Jonathan Papa University of Rochester Central Objectives: The research involves a revelation of the solution space for revolutionary families of four-mirror freeform reflective imaging systems. A freeform optical system is one that lacks rotational symmetry, meaning there is no constraint on the surface shape of the mirrors. Freeform designs can mitigate the disadvantages that prevent […]<\/p>\n","protected":false},"author":66,"featured_media":63462,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"nasa_hds_core_meta_l10n":"en-US","nasa_hds_core_meta_article_editor":"","nasa_hds_core_meta_article_contacts":[],"nasa_hds_core_meta_article_topic":"","nasa_hds_core_meta_linked_locations":[],"nasa_hds_core_meta_article_related_articles":[],"hds_migrate_meta_pr_release_id":"","hds_migrate_meta_pr_release_type":"","nasa_hds_core_meta_location_x":"","nasa_hds_core_meta_location_y":"","nasa_hds_core_meta_gallery_images":[],"footnotes":""},"categories":[3337],"news-tags":[],"internal-terms":[9529,12750],"coauthors":[],"parsely":{"version":"1.1.0","meta":{"@context":"https:\/\/schema.org","@type":"NewsArticle","headline":"Four-Mirror Freeform Reflective Imaging Systems","url":"https:\/\/www.nasa.gov\/directorates\/stmd\/space-tech-research-grants\/four-mirror-freeform-reflective-imaging-systems\/","mainEntityOfPage":{"@type":"WebPage","@id":"https:\/\/www.nasa.gov\/directorates\/stmd\/space-tech-research-grants\/four-mirror-freeform-reflective-imaging-systems\/"},"thumbnailUrl":"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?w=150&h=150&crop=1","image":{"@type":"ImageObject","url":"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg"},"articleSection":"NASA Directorates","author":[{"@type":"Person","name":"Loura Hall"}],"creator":["Loura Hall"],"publisher":{"@type":"Organization","name":"NASA","logo":"https:\/\/www.nasa.gov\/wp-content\/themes\/nasa\/assets\/images\/nasa-logo.svg"},"keywords":["NASA Directorates","Space Technology Mission Directorate","Space Technology Research Grants"],"dateCreated":"2016-07-19T19:12:00Z","datePublished":"2016-07-19T19:12:00Z","dateModified":"2023-07-26T19:12:59Z"},"rendered":"<meta name=\"parsely-title\" content=\"Four-Mirror Freeform Reflective Imaging Systems\" \/>\n<meta name=\"parsely-link\" content=\"https:\/\/www.nasa.gov\/directorates\/stmd\/space-tech-research-grants\/four-mirror-freeform-reflective-imaging-systems\/\" \/>\n<meta name=\"parsely-type\" content=\"post\" \/>\n<meta name=\"parsely-image-url\" content=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg?w=150&h=150&crop=1\" \/>\n<meta name=\"parsely-pub-date\" content=\"2016-07-19T19:12:00Z\" \/>\n<meta name=\"parsely-section\" content=\"NASA Directorates\" \/>\n<meta name=\"parsely-tags\" content=\"NASA Directorates,Space Technology Mission Directorate,Space Technology Research Grants\" \/>\n<meta name=\"parsely-author\" content=\"Loura Hall\" \/>","tracker_url":"https:\/\/cdn.parsely.com\/keys\/nasa.gov\/p.js"},"read_time":3,"time_ago":"8 years","featured_image":{"id":63462,"file":"https:\/\/www.nasa.gov\/wp-content\/uploads\/2016\/06\/papa_jonathan.jpg","title":"ImageJ=1.45s","alt":"Jonathan Papa","caption":"ImageJ=1.45s"},"_links":{"self":[{"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/posts\/61368"}],"collection":[{"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/users\/66"}],"replies":[{"embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/comments?post=61368"}],"version-history":[{"count":1,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/posts\/61368\/revisions"}],"predecessor-version":[{"id":463516,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/posts\/61368\/revisions\/463516"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/media\/63462"}],"wp:attachment":[{"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/media?parent=61368"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/categories?post=61368"},{"taxonomy":"news-tags","embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/news-tags?post=61368"},{"taxonomy":"internal-terms","embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/internal-terms?post=61368"},{"taxonomy":"author","embeddable":true,"href":"https:\/\/www.nasa.gov\/wp-json\/wp\/v2\/coauthors?post=61368"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}