{"id":7418,"date":"2023-08-15T20:42:36","date_gmt":"2023-08-15T20:42:36","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7418"},"modified":"2023-08-15T20:42:36","modified_gmt":"2023-08-15T20:42:36","slug":"ero2-0-modelling-of-the-effects-of-surface-roughness-on-molybdenum-erosion-and-redeposition-in-the-psi-2-linear-plasma-device","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/ero2-0-modelling-of-the-effects-of-surface-roughness-on-molybdenum-erosion-and-redeposition-in-the-psi-2-linear-plasma-device\/","title":{"rendered":"ERO2.0 modelling of the effects of surface roughness on molybdenum erosion and redeposition in the PSI-2 linear plasma device"},"content":{"rendered":"<p>The surface morphology of plasma-facing components (PFCs) and its evolution during plasma irradiation has been shown to have a significant effect on the erosion and subsequent transport of sputtered particles in plasma. This in turn can influence the resulting lifetime of PFCs. A model for treatment of the effect of surface roughness on the erosion of PFCs has recently been incorporated into the three-dimensional Monte Carlo code ERO2.0. First simulations have confirmed a significant influence of the assumed surface roughness (for both regular and stochastic numerically constructed samples) on both the effective sputtering yields Y-eff and the effective angular distributions of sputtered particles. In this study, a series of experiments at the linear plasma device PSI-2 are conducted to test the effect of surface roughness on the sputtering parameters. Graphite samples prepared with a 100 nm molybdenum layer with various surface roughness characteristic sizes (R-a = 110 nm, 280 nm, 600 nm and R-a < 20 nm) were exposed to a helium plasma in the PSI-2 linear plasma device at a magnetic field B.=.0.1 T. These PSI-2 experiments were simulated using ERO2.0 with a surface morphology model. Simulations are able to reproduce the experimentally observed significant suppression of erosion for higher R-a values.\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Eksaeva A.; Borodin D.; Romazanov J.; Kreter A.; Pospieszczyk A.; Dickheuer S.; M\u00f6ller S.; G\u00f6ths B.; Rasinski M.; Knoche U.; Terra A.; Kirschner A.; Borodkina I.; Eichler M.; Unterberg B.; Brezinsek S.; Linsmeier Ch.; Vassallo E.;  Pedroni M.; Passoni M.; Dellasega D.; Sala M.; Romeo F.; Henderson S.; MO&#8217;Mullane M.; Summers H.; Tskhakaya D.; Schmid K.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[574],"product_tag":[2431,2517,2518,2519,2520,2521,2522],"class_list":["post-7418","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-sputtering","product_tag-surface-morphology","product_tag-3d-monte-carlo-ero","product_tag-linear-plasma-device","product_tag-molybdenum","product_tag-surface-roughness","product_tag-ero2-0","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7418","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=7418"}],"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=7418"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7418"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7418"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}