{"id":749,"date":"2016-03-10T11:00:35","date_gmt":"2016-03-10T11:00:35","guid":{"rendered":"http:\/\/heidib.me\/cyclotron\/?page_id=749"},"modified":"2016-03-10T14:23:57","modified_gmt":"2016-03-10T14:23:57","slug":"12-inch-cyclotron-phosphor-screens","status":"publish","type":"page","link":"http:\/\/koethcyclotron.org\/?page_id=749","title":{"rendered":"12 Inch Cyclotron Phosphor Screens"},"content":{"rendered":"<p><span style=\"font-size: small;\">This is a pictorial history of the phosphor screens used in our cyclotron.<\/span><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_1.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_1.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 1 First phosphor screen we used, ZnS with Au coating<\/p><\/div>\n<div style=\"width: 246px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_2.jpg\"><img loading=\"lazy\" src=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_2.jpg?resize=236%2C400\" alt=\"\" width=\"236\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 2 First beam spot photographed (Sept 16, 1999)<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_3.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_3.jpg?resize=400%2C390\" alt=\"\" width=\"400\" height=\"390\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 3 Spot from chimney based ion source<\/p><\/div>\n<div style=\"width: 403px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_4.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_4.jpg?resize=393%2C400\" alt=\"\" width=\"393\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 4 vertical betatron motion captured<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_5.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_5.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 5 Damage to ZnS screen<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_6.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_6.jpg?resize=400%2C266\" alt=\"\" width=\"400\" height=\"266\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 6 Home made P22 Phosphor screens ! Very uniform coating.<\/p><\/div>\n<div style=\"width: 336px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_7.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_7.jpg?resize=326%2C400\" alt=\"\" width=\"326\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 7 The P22 phosphor screen can resolve individual turns<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_8.jpg\"><img loading=\"lazy\" src=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_8.jpg?resize=400%2C266\" alt=\"\" width=\"400\" height=\"266\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 8 The beam was so intense the the P22 illuminated Tim's face through a viewport<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_9.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_9.jpg?resize=400%2C382\" alt=\"\" width=\"400\" height=\"382\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 9 Damage to P22 screen slightly visible under room light<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_10.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_10.jpg?resize=400%2C266\" alt=\"\" width=\"400\" height=\"266\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 10 Damage to P22 screen obvious under UV light<\/p><\/div>\n<p>&nbsp;<\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_11.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_11.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 11 Location of beam deflector system in chamber<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_12.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_12.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 12 Beam terminates on phosphor screen at end of deflection channel<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_13.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_13.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 13 View of phosphor screen at end of deflection channel<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_14.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_14.jpg?resize=400%2C266\" alt=\"\" width=\"400\" height=\"266\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 14 We've devised a universal mounting system to accommodate many phosphor plates<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_15.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_15.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 15 Assortment of phosphor plate arrangements under room light<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_15a.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_15a.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 16 Assortment of phosphor plate arrangements under UV light<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_16.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_16.jpg?resize=400%2C262\" alt=\"\" width=\"400\" height=\"262\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 17 View of phosphor screen at end of deflection channel under room light<\/p><\/div>\n<div style=\"width: 401px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_17.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_17.jpg?resize=391%2C400\" alt=\"\" width=\"391\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 18 Cyclotron is on: halo indicates beam is approaching...<\/p><\/div>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_18.jpg\"><img loading=\"lazy\" src=\"https:\/\/i1.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_18.jpg?resize=400%2C395\" alt=\"\" width=\"400\" height=\"395\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 19 Intense beam on screen!<\/p><\/div>\n<p><center><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_19.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_19.jpg?resize=400%2C378\" alt=\"\" width=\"400\" height=\"378\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 20 Reducing camera exposure value<\/p><\/div>\n<p><\/center><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_19a.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_19a.jpg?resize=400%2C370\" alt=\"\" width=\"400\" height=\"370\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 21 Increasing the deflector voltage brings the beam further onto the screen<\/p><\/div>\n<div style=\"width: 379px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_20.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_20.jpg?resize=369%2C400\" alt=\"\" width=\"369\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 22 Reducing the camera's EV even more reveals beam structure (multiple turns layers)<\/p><\/div>\n<p><a href=\"http:\/\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/images\/screen_21.jpg\"><br \/>\n<\/a><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_21.jpg\"><img loading=\"lazy\" src=\"https:\/\/i2.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_21.jpg?resize=400%2C266\" alt=\"\" width=\"400\" height=\"266\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 23 Damage to P22 screen slightly visible under room light<\/p><\/div>\n<p><a href=\"http:\/\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/images\/screen_22.jpg\"><br \/>\n<\/a><\/p>\n<div style=\"width: 276px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_22.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_22.jpg?resize=266%2C400\" alt=\"\" width=\"266\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 24 Damage to P22 screen is obvious under UV light<\/p><\/div>\n<p><a href=\"http:\/\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/images\/screen_23.jpg\"><br \/>\n<\/a><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_23.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_23.jpg?resize=400%2C300\" alt=\"\" width=\"400\" height=\"300\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 25 A plate to test 6 different phosphors at once<\/p><\/div>\n<div style=\"width: 387px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_24.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_24.jpg?resize=377%2C400\" alt=\"\" width=\"377\" height=\"400\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 26 Multi-phosphor plate under 10 keV X-ray beam<\/p><\/div>\n<p><a href=\"http:\/\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/images\/screen_25.jpg\"><br \/>\n<\/a><\/p>\n<div style=\"width: 410px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_25.jpg\"><img loading=\"lazy\" src=\"https:\/\/i0.wp.com\/www.physics.rutgers.edu\/cyclotron\/images\/screens\/thumbnails\/screen_25.jpg?resize=400%2C389\" alt=\"\" width=\"400\" height=\"389\" border=\"0\" data-recalc-dims=\"1\" \/><\/a><p class=\"wp-caption-text\">Fig. 27 Multi-phosphor plate under 250 keV ion beam<\/p><\/div>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>This is a pictorial history of the phosphor screens used in our cyclotron. &nbsp; &nbsp;<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"spay_email":""},"jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/P6SHXY-c5","_links":{"self":[{"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/pages\/749"}],"collection":[{"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=749"}],"version-history":[{"count":5,"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/pages\/749\/revisions"}],"predecessor-version":[{"id":755,"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=\/wp\/v2\/pages\/749\/revisions\/755"}],"wp:attachment":[{"href":"http:\/\/koethcyclotron.org\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=749"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}