{"id":304266,"date":"2016-09-16T17:00:00","date_gmt":"2016-09-16T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=3c6e345080b4c57c7f3c998e3ec475f5"},"modified":"2016-09-16T17:00:00","modified_gmt":"2016-09-16T14:00:00","slug":"high-brightness-high-energy-electron-beams-from-a-laser-wakefield-accelerator-via-energy-chirp-control","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=304266","title":{"rendered":"High-Brightness High-Energy Electron Beams from a Laser Wakefield Accelerator via Energy Chirp Control"},"content":{"rendered":"<p>Author(s): W.\u2009T. Wang, W.\u2009T. Li, J.\u2009S. Liu, Z.\u2009J. Zhang, R. Qi, C.\u2009H. Yu, J.\u2009Q. Liu, M. Fang, Z.\u2009Y. Qin, C. Wang, Y. Xu, F.\u2009X. Wu, Y.\u2009X. Leng, R.\u2009X. Li, and Z.\u2009Z. Xu<\/p>\n<p>Using a new two-stage acceleration scheme, where electron injection and seeding are controlled in different periods of the laser wakefield, high-quality tunable electron beams are produced with brightnesses close to those achieved in state-of-the-art linac drivers.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.124801.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 117, 124801] Published Fri Sep 16, 2016<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): W.&thinsp;T. Wang, W.&thinsp;T. Li, J.&thinsp;S. Liu, Z.&thinsp;J. Zhang, R. Qi, C.&thinsp;H. Yu, J.&thinsp;Q. Liu, M. Fang, Z.&thinsp;Y. Qin, C. Wang, Y. Xu, F.&thinsp;X. Wu, Y.&thinsp;X. Leng, R.&thinsp;X. Li, and Z.&thinsp;Z. Xu<\/p>\n<p>Using a new two-stage acceleration scheme, where electron injection and seeding are controlled in different periods of the laser wakefield, high-quality tunable electron beams are produced with brightnesses close to those achieved in state-of-the-art linac drivers.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.124801.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 117, 124801] Published Fri Sep 16, 2016<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[182],"tags":[],"class_list":{"0":"post-304266","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-teadus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/304266","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=304266"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/304266\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=304266"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=304266"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=304266"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}