{"id":7186,"date":"2023-07-20T14:44:24","date_gmt":"2023-07-20T14:44:24","guid":{"rendered":"https:\/\/er-c.org\/?page_id=7186"},"modified":"2023-07-20T16:05:33","modified_gmt":"2023-07-20T16:05:33","slug":"sample-preparation-fib","status":"publish","type":"page","link":"https:\/\/er-c.org\/index.php\/facilities-2\/facilities-material-science\/sample-preparation\/sample-preparation-fib\/","title":{"rendered":"Sample Preparation FIB"},"content":{"rendered":"\n<figure class=\"wp-block-image size-large is-resized\"><img decoding=\"async\" src=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-1024x171.png\" alt=\"\" class=\"wp-image-7229\" width=\"1200\" srcset=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-1024x171.png 1024w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-300x50.png 300w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-768x128.png 768w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-1536x257.png 1536w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/FIB-1-2048x343.png 2048w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n<div\n\t\t\t\n\t\t\tclass=\"so-widget-sow-headline so-widget-sow-headline-default-e68cdc7fd8ad\"\n\t\t\t\n\t\t><div class=\"sow-headline-container \">\n\t\t\t\t\t\t\t<h1 class=\"sow-headline\">\n\t\t\t\t\t\tFocused Ion Beam Sample Preparation\t\t\t\t\t\t<\/h1>\n\t\t\t\t\t\t<\/div>\n<\/div>\n\n\n<hr>\n<p style=\"text-align: center;\">In contrast to time-consuming conventional TEM-specimen preparation methods, the focused ion beam (FIB) sputtering in a dual beam SEM system allows to produce high-quality specimens for various TEM studies in a (semi-)automated and much quicker way (within several hours). Modern dual beam FIB\/SEMs use precise piezo-controlled manipulators, various gas injection systems to protect the sample surface, energy dispersive X-ray spectroscopy to measure composition and different detectors to image the specimen during the preparation process. In the dual systems, the imaging process results from using&nbsp; scanning electrons (SEM) whereby scanning of focused gallium ions at the sample surface enables local material abrasion.<\/p>\n\n\n\n<hr \/>\n\n\n\n<div style=\"height:20px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n<div id=\"pl-gb7186-69d61073eaa34\"  class=\"panel-layout\" ><div id=\"pg-gb7186-69d61073eaa34-0\"  class=\"panel-grid panel-has-style\" ><div class=\"panel-row-style panel-row-style-for-gb7186-69d61073eaa34-0\" ><div id=\"pgc-gb7186-69d61073eaa34-0-0\"  class=\"panel-grid-cell\" ><div id=\"panel-gb7186-69d61073eaa34-0-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child widgetopts-SO\" data-index=\"0\" ><div\n\t\t\t\n\t\t\tclass=\"so-widget-sow-editor so-widget-sow-editor-base\"\n\t\t\t\n\t\t><h3 class=\"widget-title\">Helios Nanolab FIB<\/h3>\n<div class=\"siteorigin-widget-tinymce textwidget\">\n\t<p>The standard TEM-lamella preparation (lift-out method) process consists of depositing a protective layer (e.g. Pt, C, W), cutting the slice perpendicular to the surface (cross-section preparation), lifting out of the slice with the help of a micromanipulator, attaching the specimen to a TEM support grid made of Cu or Mo, and finally polishing the lamella to the desired dimensions and thicknesses. Variations of both, the accelerating voltage (typically 5 \u2013 30 keV) and beam current (2,8 nA \u2013 48 pA) make the FIB\/SEM systems able to prepare ultra-thin TEM-specimens from almost any materials in solid form ranging from metals to soft matter.<\/p>\n<p>At the ER-C we work with a <strong><a href=\"https:\/\/er-c.org\/index.php\/facilities-2\/facilities-material-science\/material-science\/fei-helios-nanolab-400s-fib-sem\/\">Helios NanoLab 400S<\/a><\/strong> and a <strong><a href=\"https:\/\/er-c.org\/index.php\/facilities-2\/facilities-material-science\/material-science\/fei-helios-nanolab-460f1-fib-sem\/\">Helios NanoLab 460F1<\/a>.<\/strong><\/p>\n<p>&nbsp;<\/p>\n<\/div>\n<\/div><\/div><\/div><div id=\"pgc-gb7186-69d61073eaa34-0-1\"  class=\"panel-grid-cell\" ><div id=\"panel-gb7186-69d61073eaa34-0-1-0\" class=\"so-panel widget widget_media_image panel-first-child panel-last-child widgetopts-SO\" data-index=\"1\" ><img loading=\"lazy\" decoding=\"async\" width=\"900\" height=\"676\" src=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-1024x769.jpg\" class=\"image wp-image-7157  attachment-large size-large\" alt=\"\" style=\"max-width: 100%; height: auto;\" srcset=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-1024x769.jpg 1024w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-300x225.jpg 300w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-768x576.jpg 768w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-1536x1153.jpg 1536w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fib_460_er_c_1_02-2048x1537.jpg 2048w\" sizes=\"auto, (max-width: 900px) 100vw, 900px\" \/><\/div><\/div><\/div><\/div><div id=\"pg-gb7186-69d61073eaa34-1\"  class=\"panel-grid panel-has-style\" ><div class=\"panel-row-style panel-row-style-for-gb7186-69d61073eaa34-1\" ><div id=\"pgc-gb7186-69d61073eaa34-1-0\"  class=\"panel-grid-cell\" ><div id=\"panel-gb7186-69d61073eaa34-1-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child widgetopts-SO\" data-index=\"2\" ><div\n\t\t\t\n\t\t\tclass=\"so-widget-sow-editor so-widget-sow-editor-base\"\n\t\t\t\n\t\t><h3 class=\"widget-title\">Fischione Nanomill\u00ae<\/h3>\n<div class=\"siteorigin-widget-tinymce textwidget\">\n\t<p>The Fischione Nanomill\u00ae is a low-energy focused Ar ion (&lt;1 keV) milling system dedicated for removal of the FIB-induced damage layer from TEM lamellae. The scanning ion beam provides images based on secondary electrons, which help to focus the sputtering process exclusively on the FIB-prepared lamella. The system is equipped with liquid nitrogen cooling dedicated for sputtering of sensitive materials. The parameters of the ion milling process can be individually fitted to the sample material and aim of the TEM experiment.<\/p>\n<p>Reference: doi:10.1017\/S1431927617000514<\/p>\n<\/div>\n<\/div><\/div><\/div><div id=\"pgc-gb7186-69d61073eaa34-1-1\"  class=\"panel-grid-cell\" ><div id=\"panel-gb7186-69d61073eaa34-1-1-0\" class=\"so-panel widget widget_media_image panel-first-child panel-last-child widgetopts-SO\" data-index=\"3\" ><img loading=\"lazy\" decoding=\"async\" width=\"900\" height=\"676\" src=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-1024x769.jpg\" class=\"image wp-image-7225  attachment-large size-large\" alt=\"\" style=\"max-width: 100%; height: auto;\" srcset=\"https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-1024x769.jpg 1024w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-300x225.jpg 300w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-768x576.jpg 768w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-1536x1153.jpg 1536w, https:\/\/er-c.org\/wp-content\/uploads\/2023\/07\/fischione_nanomill_er_c_1_01-2048x1537.jpg 2048w\" sizes=\"auto, (max-width: 900px) 100vw, 900px\" \/><\/div><\/div><\/div><\/div><\/div>\n\n\n<div style=\"height:20px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n","protected":false},"excerpt":{"rendered":"<p>In contrast to time-consuming conventional TEM-specimen preparation methods, the focused ion beam (FIB) sputtering in a dual beam SEM system allows to produce high-quality specimens for various TEM studies in a (semi-)automated and much quicker way (within several hours). Modern dual beam FIB\/SEMs use precise piezo-controlled manipulators, various gas injection systems to protect the sample surface, energy dispersive X-ray spectroscopy to measure composition and different detectors to image the specimen during the preparation process. In the dual systems, the imaging process results from using\u00a0 scanning electrons (SEM) whereby scanning of focused gallium ions at the sample surface enables local material abrasion.<\/p>\n","protected":false},"author":2,"featured_media":7226,"parent":7171,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"page-templates\/pagebuilder.php","meta":{"_themeisle_gutenberg_block_has_review":false,"footnotes":""},"class_list":["post-7186","page","type-page","status-publish","has-post-thumbnail","hentry"],"_links":{"self":[{"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/pages\/7186","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/comments?post=7186"}],"version-history":[{"count":3,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/pages\/7186\/revisions"}],"predecessor-version":[{"id":7230,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/pages\/7186\/revisions\/7230"}],"up":[{"embeddable":true,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/pages\/7171"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/media\/7226"}],"wp:attachment":[{"href":"https:\/\/er-c.org\/index.php\/wp-json\/wp\/v2\/media?parent=7186"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}