Fluid Modelling of Hollow Cathode Copper Ion Laser with Cathode Sputtering

2019 ◽  
Author(s):  
Danka Yordanova ◽  
Margarita Grozeva ◽  
Diana Mihailova ◽  
Jan van Dijk
1984 ◽  
Vol 51 (6) ◽  
pp. 417-419 ◽  
Author(s):  
M. Grozeva ◽  
N. Sabotinov

2003 ◽  
Author(s):  
Diana B. Mihailova ◽  
Margarita G. Grozeva ◽  
Annemie Bogaerts ◽  
R. H. Gijbels ◽  
Nikola V. Sabotinov

1994 ◽  
Vol 27 (2) ◽  
pp. 219-227 ◽  
Author(s):  
K A Peard ◽  
K Rozsa ◽  
R C Tobin

1981 ◽  
Author(s):  
H. Koch ◽  
W. Wittwer

2005 ◽  
Vol 862 ◽  
Author(s):  
R. J. Soukup ◽  
N. J. Ianno ◽  
J. S. Schrader ◽  
V. L. Dalal

AbstractExperimental results on thin films of the new material GexC1-x, deposited by a unique dual plasma hollow cathode sputtering technique are presented. The mostimportant contribution of this work is that it shows that by using non-equilibrium growth conditions resulting from the hollow cathode technique, one can grow Group IV materials which cannot otherwise be grown using normal CVD or MBE processes. The sputtering is accomplished by igniting a dc plasma in the Ar and H2 gases which are fed through Ge and C nozzles.The GeC films are grown on etched Si (100), on Si with the native oxide and on glass. The films grown on glass were quite disordered, but the films grown on both types of Si substrates were very ordered in nature. This order has been characterized using Xray diffraction (XRD) and Raman spectroscopy.Films with as much as 8% C have been deposited. In order to produce useful GexC1-x films, the C must bond to the Ge at lattice sites. Evidence of this desired GeC bond has been seen using Fourier Transform Infrared Spectroscopy (FTIR), Raman Spectroscopy, and XRD.


Coatings ◽  
2018 ◽  
Vol 8 (9) ◽  
pp. 303 ◽  
Author(s):  
Sergey Grigoriev ◽  
Alexander Metel ◽  
Marina Volosova ◽  
Yury Melnik

A new hollow cathode sputtering system is used for beam-assisted deposition of thin films on dielectric substrates. A copper target placed at the hollow cathode bottom is uniformly sputtered by argon ions from the glow discharge plasma filling the cathode. Through an emissive grid, sputtered copper atoms leave the cathode together with accelerated argon ions. On their way to the substrate, the ions—due to charge exchange collisions—turn into fast argon atoms bombarding the growing film. With increasing argon ion energy, continuous bombardment results in the film adhesion improvement and reduction of the deposition rate down to zero, at an energy of about 2 keV. The pulsed bombardment does not influence the film deposition rate, and results in a monotonic growth of the film adhesion up to 20 MPa when increasing the fast atom energy up to 10 keV.


1999 ◽  
Author(s):  
Jianhua Yu ◽  
Jianjun Huang ◽  
Jingzhen Li
Keyword(s):  

2016 ◽  
Vol 120 (4) ◽  
pp. 044308 ◽  
Author(s):  
Rickard Gunnarsson ◽  
Iris Pilch ◽  
Robert D. Boyd ◽  
Nils Brenning ◽  
Ulf Helmersson

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