{"id":81,"date":"2021-02-12T08:32:44","date_gmt":"2021-02-12T08:32:44","guid":{"rendered":"https:\/\/e-rihs.cz\/wp\/?page_id=81"},"modified":"2021-02-12T08:32:44","modified_gmt":"2021-02-12T08:32:44","slug":"tandetron-laboratory","status":"publish","type":"page","link":"https:\/\/e-rihs.cz\/wp\/?page_id=81","title":{"rendered":"Tandetron Laboratory"},"content":{"rendered":"<p><strong>Tandetron Laboratory (NPI)<\/strong><\/p>\n<ul>\n<li>Tandetron 4130 MC \u2013 a compact, multipurpose electrostatic tandem accelerator system with terminal voltage varying from 200 kV to 3 MV; ion beams with energies ranging from 400 keV to 24 MeV of almost all elements of the periodic system, ion currents from nA to microA.<\/li>\n<li>Rutherford Back-Scattering spectrometry (RBS), a high sensitivity for heavy elements, low detection limit and about 10 nm depth resolution in elemental depth profiling.<\/li>\n<li>Elastic Recoil Detection Analysis (ERDA), non-destructive depth profiling of light elements in bulk samples.<\/li>\n<li>Time of Flight (TOF)-ERDA, distinguishes the outgoing light ions and recoiled atoms according to their mass.<\/li>\n<li>Particle Induced X-Ray Emission spectroscopy (PIXE), light elements analysis with a high sensitivity detection limit down to 1 ppm.<\/li>\n<li>Particle Induced Gamma-Ray Emission spectroscopy (PIGE), light elements analysis with a detection limit up to 1000 ppm.<\/li>\n<li>External beam, investigation of samples unstable under vacuum conditions, biological samples or samples too large to be mounted in a vacuum chamber.<\/li>\n<li>Ion Micro-beam, focusing on an ion beam to dimensions of about 1\u00b5m scanning on a sample, a versatile piece of equipment that allows 3D elemental mapping of microstructures.<\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>Tandetron Laboratory (NPI) Tandetron 4130 MC \u2013 a compact, multipurpose electrostatic tandem accelerator system with terminal voltage varying from 200 kV to 3 MV; ion beams with energies ranging from 400 keV to 24 MeV of almost all elements of the periodic system, ion currents from nA to microA. Rutherford Back-Scattering spectrometry (RBS), a high [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":65,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"_links":{"self":[{"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/pages\/81"}],"collection":[{"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=81"}],"version-history":[{"count":1,"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/pages\/81\/revisions"}],"predecessor-version":[{"id":82,"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/pages\/81\/revisions\/82"}],"up":[{"embeddable":true,"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=\/wp\/v2\/pages\/65"}],"wp:attachment":[{"href":"https:\/\/e-rihs.cz\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=81"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}