{"id":517,"date":"2017-06-17T18:36:49","date_gmt":"2017-06-17T22:36:49","guid":{"rendered":"http:\/\/phy.sites.mtu.edu\/yap\/?p=517"},"modified":"2017-06-17T18:36:49","modified_gmt":"2017-06-17T22:36:49","slug":"growth-of-adhesive-cubic-phase-boron-nitride-films-without-argon-ion-bombardment","status":"publish","type":"post","link":"http:\/\/phy.sites.mtu.edu\/yap\/2017\/06\/17\/growth-of-adhesive-cubic-phase-boron-nitride-films-without-argon-ion-bombardment\/","title":{"rendered":"Growth of adhesive cubic phase boron nitride films  without argon ion bombardment"},"content":{"rendered":"<p><a href=\"http:\/\/phy.sites.mtu.edu\/yap\/wp-content\/uploads\/2017\/06\/Cubic-BN-DMR2006.pdf\">Cubic-BN-DMR2006<\/a><\/p>\n<p>Previously, in situ bombardment of massive ions (Ar+, Kr+, etc.) was considered to be necessary for the formation of c-BN films. Because of<\/p>\n<p>the accumulated stress, bombardment of massive ions has led to the formation of c-BN films with poor adhesion. Here we show that c-BN films<\/p>\n<p>can be grown without involving bombardment of massive ions. This is achieved by using plasma-assisted pulsed-laser deposition (PLD) in pure<\/p>\n<p>N2 RF plasma. Furthermore, we show that c-BN films can be grown in a vacuum ( \u0308105 mbar during growth) by PLD without auxiliary ion<\/p>\n<p>source. We show that these are possible at a reduced deposition rate. Energetic growth species initiated by PLD and the pure N2 plasma is<\/p>\n<p>sufficient to form adhesive c-BN films at moderate deposition rate as long as the energy transfer rate per growth species is sufficient.<\/p>\n<p>D 2005 Elsevier B.V. All rights reserved.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Cubic-BN-DMR2006 Previously, in situ bombardment of massive ions (Ar+, Kr+, etc.) was considered to be necessary for the formation of c-BN films. Because of the accumulated stress, bombardment of massive ions has led to the formation of c-BN films with poor adhesion. Here we show that c-BN films can be grown without involving bombardment of [&hellip;]<\/p>\n","protected":false},"author":4,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[60,87,89,99,98,97],"tags":[],"class_list":["post-517","post","type-post","status-publish","format-standard","hentry","category-60","category-boron","category-boronnitride","category-cubic-phase","category-films","category-ion"],"_links":{"self":[{"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/posts\/517","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/comments?post=517"}],"version-history":[{"count":1,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/posts\/517\/revisions"}],"predecessor-version":[{"id":519,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/posts\/517\/revisions\/519"}],"wp:attachment":[{"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/media?parent=517"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/categories?post=517"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/phy.sites.mtu.edu\/yap\/wp-json\/wp\/v2\/tags?post=517"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}