{"id":77,"date":"2024-10-02T21:01:05","date_gmt":"2024-10-02T21:01:05","guid":{"rendered":"https:\/\/wpw.bnl.gov\/nsrl\/?page_id=77"},"modified":"2025-02-27T19:47:42","modified_gmt":"2025-02-27T19:47:42","slug":"spatial-characteristics","status":"publish","type":"page","link":"https:\/\/wpw.bnl.gov\/nsrl\/beam\/spatial-characteristics\/","title":{"rendered":"Spatial Characteristics"},"content":{"rendered":"\n<p>As particles travel down the NSRL beamline, magnetic lenses steer and shape them before they exit the vacuum window and enter the <a href=\"https:\/\/wpw.bnl.gov\/nsrl\/target-room\/\" data-type=\"page\" data-id=\"42\">target room<\/a>. These magnets effectively distribute the particles into a particular pattern of high intensity and low intensity regions across the plane perpendicular to the particles&#8217; axis of travel. This distribution is referred to as the &#8220;beam shape&#8221;, &#8220;beam spot&#8221;, or &#8220;beam profile&#8221;. An image depicting one such beam profile as captured by the NSRL digital beam imager is shown below.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img decoding=\"async\" src=\"https:\/\/wpw.bnl.gov\/nsrl\/wp-content\/uploads\/sites\/15\/2024\/11\/example_beam6_wide.svg\" alt=\"\" class=\"wp-image-930\" \/><\/figure>\n\n\n\n<p>The areas corresponding to higher intensity appear as a lighter color, and those with lower intensity appear as a darker color, corresponding to the color scale on the right. The intensity is given in arbitrary units. 8 fiducial corner marks can be seen. The inner 4 represent a square with 10 cm (3.9 inch) sides, and the outer 4 represent a square with 20 cm (7.9 inch) sides.<\/p>\n\n\n\n<p>The NSRL beamline&#8217;s magnetic optics allow a fairly unique beam shape to be produced. Two octupole magnets can bend the tails of a gaussian-profile beam in towards the center. The resultant profile has a large rectangular uniform region, surrounded by high intensity &#8220;ears&#8221; at the edges.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\" id=\"square-beam\">Square Beam<\/h2>\n\n\n\n<p>Although the beam profile at NSRL can be tuned to a variety of shapes and sizes, the most common profiles used in physics or electronics testing experiments are &#8220;square&#8221; beams with a uniform center of 20\u00d720 cm<sup>2<\/sup> or 7\u00d77 cm<sup>2<\/sup>. Other arbitrary rectangular shapes are most often achieved by collimating the beam with an <a href=\"https:\/\/wpw.bnl.gov\/nsrl\/beamline\/collimators\/#adjustable-collimator\" data-type=\"page\" data-id=\"103\">adjustable tungsten collimator<\/a> rather than tuning it, which allows NSRL to maintain a smaller set of well tuned and accurately calibrated beams while still permitting the beam spot to be adjusted.<\/p>\n\n\n\n<p>Specially tuned beams can be developed upon request if they are necessary for a test.<br><\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Other Beam Shapes<\/h2>\n\n\n\n<p>In addition to the larger &#8220;square&#8221; beam spots, small beam spots can be achieved for physics experiments. Although the size of the final focus depends on beam energy and ion species, typical spot sizes of 1 cm RMS can be achieved. Small spots or other beam shapes can be produced through the use of collimators. If you have any special demands, contact the <a href=\"mailto:sivertz@bnl.gov\">NSRL PI<\/a> while you are planning your experiment to ensure that the beam conditions you need will be available.<\/p>\n\n\n\n<p>While not typically used for physics or electronics testing experiments, the NSRL beamline is capable of producing an overfocused beam with a larger uniform area of up to 60\u00d760 cm<sup>2<\/sup>. These beams are not recommended for electronics testing work due to their comparatively low flux, divergent geometry, and difficulty of setup.<br><\/p>\n\n\n\n<hr \/>\n<span>This page was last modified:<\/span>\n\n\n<div class=\"wp-block-post-date__modified-date wp-block-post-date\"><time datetime=\"2025-02-27T19:47:42+00:00\">February 27, 2025<\/time><\/div>","protected":false},"excerpt":{"rendered":"<p>As particles travel down the NSRL beamline, magnetic lenses steer and shape them before they exit the vacuum window and enter the target room. These magnets effectively distribute the particles into a particular pattern of high intensity and low intensity regions across the plane perpendicular to the particles&#8217; axis of travel. This distribution is referred&hellip; <a class=\"more-link\" href=\"https:\/\/wpw.bnl.gov\/nsrl\/beam\/spatial-characteristics\/\">Continue reading <span class=\"screen-reader-text\">Spatial Characteristics<\/span><\/a><\/p>\n","protected":false},"author":16,"featured_media":0,"parent":32,"menu_order":2,"comment_status":"closed","ping_status":"closed","template":"","meta":{"inline_featured_image":false,"footnotes":""},"class_list":["post-77","page","type-page","status-publish","hentry","entry"],"_links":{"self":[{"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/pages\/77","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/users\/16"}],"replies":[{"embeddable":true,"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/comments?post=77"}],"version-history":[{"count":39,"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/pages\/77\/revisions"}],"predecessor-version":[{"id":1637,"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/pages\/77\/revisions\/1637"}],"up":[{"embeddable":true,"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/pages\/32"}],"wp:attachment":[{"href":"https:\/\/wpw.bnl.gov\/nsrl\/wp-json\/wp\/v2\/media?parent=77"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}