{"id":20302,"date":"2019-05-27T09:06:37","date_gmt":"2019-05-27T07:06:37","guid":{"rendered":"http:\/\/www.eli-beams.eu\/facility\/experimental-halls\/e5-electron-accelaration-laser-undulator-x-ray-source\/lux-beamline\/"},"modified":"2023-08-29T20:03:29","modified_gmt":"2023-08-29T18:03:29","slug":"lux-beamline","status":"publish","type":"page","link":"https:\/\/www.eli-beams.eu\/facility\/experimental-halls\/e5-electron-accelaration-laser-undulator-x-ray-source\/lux-beamline\/","title":{"rendered":"LUIS Beamline"},"content":{"rendered":"<p>The LUIS technology is based on the achievements of the LUX collaboration between <a href=\"https:\/\/www.uni-hamburg.de\/\">University of Hamburg<\/a> (Germany) and ELI-Beamlines (http:\/lux.cfel.de).<\/p>\n<p>The LUIS team (leader: Dr A.Molodozhentsev) is a part of Department of 86 (head of department: Prof. S.Bulanov) is working in tight collaboration with all technical teams of ELI-Beamlines as well as the <a href=\"https:\/\/www.eli-beams.eu\/facility\/experimental-halls\/e5-electron-accelaration-laser-undulator-x-ray-source\/electron-beam-accelerator-for-fundamental-sciences-and-applications-eli-elba\/\">ELBA<\/a> and <a href=\"https:\/\/www.eli-beams.eu\/cs\/o-eli-beamlines\/projekty\/probihajici-projekty\/hifi\/\">HiFI<\/a> research teams. The LUIS team established the international collaboration with <a href=\"https:\/\/www.uni-hamburg.de\/\">University of Hamburg<\/a> (Germany), <a href=\"https:\/\/www.desy.de\/\">DESY<\/a> (Germany), <a href=\"https:\/\/www.osaka-u.ac.jp\/en\">University of Osaka<\/a> (Japan), <a href=\"https:\/\/www.qst.go.jp\/site\/kansai-english\/\">Kansai Photon Science Institute<\/a> (Nara, Japan), <a href=\"https:\/\/www.royalholloway.ac.uk\/\">Royal Holloway and Bedford New College<\/a> (United Kingdom), <a href=\"http:\/\/pwr.edu.pl\/en\/\">Wroclaw University of Science and Technology<\/a> (Poland) as well as with Czech Universities. The LUIS team is a part of the <a href=\"http:\/\/www.eupraxia-project.eu\">EuPRAXIA<\/a> international community.<\/p>\n<p>The first goal of LUIS development is characterization of the electron beam parameters, accelerated by the \u201c100TW\u201d-scale laser power (with the repetition rate up to 50 Hz), required for the LUIS research program. The electron acceleration will be performed in the pre-formed plasma channel inside of the Sapphire capillary <strong>(Picture 1<\/strong>). After the first experimental campaign, the LUIS \u201cphase0\u201d setup (current status of the LUIS-phase0 technology in the <a href=\"https:\/\/www.eli-beams.eu\/facility\/experimental-halls\/e5-electron-accelaration-laser-undulator-x-ray-source\/\">E5 hall<\/a> is shown in <strong>Picture 2<\/strong>) will be upgraded to the \u201cphase1\u201d (<strong>Picture 3<\/strong>), which includes the electron beam transport with electron beam diagnostics and the compact undulator, based on the permanent magnet technology (<strong>Picture 4<\/strong>). All key elements of the LUIS \u201cphase1\u201d setup are ready to be installed. After the successful realization of the LUIS \u201cphase1\u201d research program, the LUIS setup will be upgraded \u201cstep-by-step\u201d to the \u201cphase4\u201d final setup in order to optimize the electron beam parameters for the EUV-FEL experiments. The model of the \u201cLUIS \u201cphase4\u201d setup is presented in <strong>Picture 5<\/strong>.<\/p>\n<p>As the result of the LUIS-Phase1 setup commissioning using the <a href=\"https:\/\/www.eli-beams.eu\/facility\/lasers\/laser-3-hapls-1-pw-30-j-10-hz\/\">HAPLS laser<\/a> (adapted to the LUIS setup), the photon user community will have an assess to the LUIS photon beam with the parameters, summarized in <strong>Table 1<\/strong>. The high repetition rate operation of the LUIS setup will be possible after finalization of the <a href=\"https:\/\/www.eli-beams.eu\/facility\/lasers\/laser-2-amos-1-pw-20-j-10-hz\/\">DUHA laser<\/a> system and the L2-to-E5 laser beam transport.<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27219 \" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1L.png\" alt=\"\" width=\"226\" height=\"196\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1L.png 377w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1L-300x259.png 300w\" sizes=\"(max-width: 226px) 100vw, 226px\" \/> <img loading=\"lazy\" class=\"alignnone wp-image-27221 \" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1P-300x147.png\" alt=\"\" width=\"400\" height=\"196\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1P-300x147.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1P-1024x503.png 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1P-768x377.png 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/1P.png 1091w\" sizes=\"(max-width: 400px) 100vw, 400px\" \/><br \/>\n<strong>Picture 1:<\/strong> Discharge in the Sapphire capillary (test setup: LUIS-Lab \/ Dr. K.Kruchinin)<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27223 size-large\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-1024x763.png\" alt=\"\" width=\"1024\" height=\"763\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-1024x763.png 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-300x224.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-768x572.png 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-1536x1145.png 1536w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/2-2048x1526.png 2048w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><br \/>\n<strong>Picture 2:<\/strong> LUIS \u201cphase0\u201d setup, assembled in the E5(LUIS) experimental area.<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27225 size-large\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-1024x214.png\" alt=\"\" width=\"1024\" height=\"214\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-1024x214.png 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-300x63.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-768x161.png 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-1536x321.png 1536w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/3-2048x429.png 2048w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><br \/>\n<strong>Picture 3:<\/strong> Model of the LUIS \u201cphase1\u201d setup to produce the incoherent photon radiation for users.<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27227 size-full\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/4.png\" alt=\"\" width=\"776\" height=\"563\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/4.png 776w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/4-300x218.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/4-768x557.png 768w\" sizes=\"(max-width: 776px) 100vw, 776px\" \/><br \/>\n<strong>Picture 4:<\/strong> Compact permanent magnets undulator (UHH-ELIBL collaboration).<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27229 size-large\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-1024x429.png\" alt=\"\" width=\"1024\" height=\"429\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-1024x429.png 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-300x126.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-768x322.png 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-1536x644.png 1536w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/5-2048x858.png 2048w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><br \/>\n<strong>Picture 5:<\/strong> Model of the LUIS \u201cphase4\u201d setup to optimize the electron beam parameters, required for the EUV free electron laser operation (integrated into the E5 experimental hall).<\/p>\n<p>&nbsp;<\/p>\n<p><strong>Table 1: <\/strong>Incoherent photon beam parameters, available for the photon user community after commissioning of the LUIS-phase1 setup<\/p>\n<p><img loading=\"lazy\" class=\"alignnone wp-image-27231 size-large\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/6-1024x681.png\" alt=\"\" width=\"1024\" height=\"681\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/6-1024x681.png 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/6-300x199.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/6-768x510.png 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/02\/6.png 1294w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><em>\u00a0<\/em><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The LUIS technology is based on the achievements of the LUX collaboration between University of Hamburg (Germany) and ELI-Beamlines (http:\/lux.cfel.de)&#8230;.<\/p>\n","protected":false},"author":1,"featured_media":36415,"parent":20298,"menu_order":256,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20302"}],"collection":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/comments?post=20302"}],"version-history":[{"count":0,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20302\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20298"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/media\/36415"}],"wp:attachment":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/media?parent=20302"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}