TY - GEN
T1 - Magnetron sputtering yield and relative factors
AU - Wang, Lifeng
AU - Wu, Zeyan
AU - Meng, Zhijun
PY - 2012
Y1 - 2012
N2 - In this work, we mainly summarize the influence of the ion bombardment cathode (target) and relative factors of magnetron sputtering yield in production thin film. Magnetron sputter deposition permits a much wider selection of film materials, produces films with higher purity and better controlled composition, provides films with greater adhesive strength and homogeneity, and permits better control of deposit thickness. Unlike most other work described about sputtering yield, sputtering for thin-film production is performed using the plasma rather than a focused ion beam. When an ion with the energy hits a surface of the target, a small fraction of the energy and momentum of the incoming ion will, through lattice collisions, be reversed and may cause ejection of surface atoms (sputtering). The average number of the atoms ejected from the cathode surface per incident ion is called the sputtering yield. The sputtering yield varies with the target material, the kind of impinging ion, and the energy of that ion. At a given ion energy, The sputtering yield increases with increasing angle of incidence up to a maximum at an angle between 55 ° and 85 ° with respect to the surface normal [1, 3].
AB - In this work, we mainly summarize the influence of the ion bombardment cathode (target) and relative factors of magnetron sputtering yield in production thin film. Magnetron sputter deposition permits a much wider selection of film materials, produces films with higher purity and better controlled composition, provides films with greater adhesive strength and homogeneity, and permits better control of deposit thickness. Unlike most other work described about sputtering yield, sputtering for thin-film production is performed using the plasma rather than a focused ion beam. When an ion with the energy hits a surface of the target, a small fraction of the energy and momentum of the incoming ion will, through lattice collisions, be reversed and may cause ejection of surface atoms (sputtering). The average number of the atoms ejected from the cathode surface per incident ion is called the sputtering yield. The sputtering yield varies with the target material, the kind of impinging ion, and the energy of that ion. At a given ion energy, The sputtering yield increases with increasing angle of incidence up to a maximum at an angle between 55 ° and 85 ° with respect to the surface normal [1, 3].
KW - Impingingion
KW - Magnetron sputter
KW - Sputtering yield
KW - Target
UR - https://www.scopus.com/pages/publications/80555148664
U2 - 10.4028/www.scientific.net/AMR.361-363.1655
DO - 10.4028/www.scientific.net/AMR.361-363.1655
M3 - 会议稿件
AN - SCOPUS:80555148664
SN - 9783037852682
T3 - Advanced Materials Research
SP - 1655
EP - 1663
BT - Natural Resources and Sustainable Development
T2 - 2011 International Conference on Energy, Environment and Sustainable Development, ICEESD 2011
Y2 - 21 October 2011 through 23 October 2011
ER -