{"id":8880,"date":"2022-09-08T10:53:34","date_gmt":"2022-09-08T10:53:34","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=8880"},"modified":"2022-11-11T08:56:58","modified_gmt":"2022-11-11T08:56:58","slug":"x-ray-measurements-reveal-the-fine-dynamics-of-current-micro-discharges-in-a-vacuum-high-voltage-experiment","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/x-ray-measurements-reveal-the-fine-dynamics-of-current-micro-discharges-in-a-vacuum-high-voltage-experiment\/","title":{"rendered":"X-RAY MEASUREMENTS REVEAL THE FINE DYNAMICS OF CURRENT MICRO-DISCHARGES IN A VACUUM HIGH VOLTAGE EXPERIMENT"},"content":{"rendered":"<p>The High Voltage Padova Test Facility (HVPTF) is an experimental device for investigating High Voltage (HV) insulation in vacuum, in support of the realization of MITICA, the prototype of a neutral beam injector for ITER. Inside a high vacuum chamber, two stainless steel electrodes, separated by a few centimetres gap, can achieve an HV difference up to 800 kV During the conditioning process of the electrodes, current microdischarges and the presence of associated X-rays are observed, along with a global increase of gas emission (H2 and CO2 are detected by the Residual Gas Analyser). Different X-rays detectors have been installed during the last five years on HVPTF, with the aim to investigate the physical processes behind the conditioning by means of X-rays analyses. In this contribution, new information provided by the different devices are presented: in particular, the identification of a fine dynamics in the micro-discharge phenomenon is shown. Moreover, the growing contribution of the vacuum chamber during the electrodes conditioning, operating as a third electrode, is investigated. A possible physical interpretation of the micro-discharge dynamics is sketched. Finally, the new set of LYSO scintillators is described and preliminary results about the recent electro-polished electrodes campaign is introduced.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Spagnolo S.; Pilan N.; De Lorenzi A.; Fontana C.; Pino F.; Cordaro L.; Croci G.; Fincato M.; Lotto L.; Mario I.; Martines E.; McCormack O.; Muraro A.; Patton T.; Rigamonti D.; Spada E.; Tardocchi M.; Zuin M.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[709],"product_tag":[868,936,937,3816,3817],"class_list":["post-8880","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-proceedings-papers","product_tag-mitica","product_tag-hvptf","product_tag-high-voltage-padova-test-facility","product_tag-vacuum-high-voltage-experiment","product_tag-x-ray-measurement","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/8880","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product"}],"about":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/types\/product"}],"replies":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/comments?post=8880"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/1294"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=8880"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=8880"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=8880"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}