Three-dimensional electromagnetic PIC model of a compact ECR plasma source

1995 ◽  
Vol 23 (4) ◽  
pp. 602-608 ◽  
Author(s):  
V.P. Gopinath ◽  
T.A. Grotjohn
1991 ◽  
Vol 237 ◽  
Author(s):  
Z. Sitar ◽  
L. S. Smith ◽  
M. J. Paisley ◽  
R. F. Davis

ABSTRACTThe morphology and interface chemistry occurring during the initial stages of growth of GaN and A1N layers has been obtained. Films were grown using gas source MBE equipment containing an ECR plasma source to activate molecular nitrogen. The experiments consisted of sequential depositions of about one monolayer thick films and XPS analysis. Evidence for silicon nitride formation on the SiC surface was obtained from the studies of both the Si oxidation states and the substrate peak intensity dependence on film thickness. The growth of GaN on sapphire appeared to occur via the Stranski-Krastanov mode, while the growth on SiC showed characteristics of three-dimensional growth. AlN grew in a layer-by-layer mode on both substrates.


2019 ◽  
Vol 85 (4) ◽  
Author(s):  
M. Magarotto ◽  
D. Melazzi ◽  
D. Pavarin

We have numerically studied how an actual confinement magnetostatic field affects power deposition in a helicon source. We have solved the wave propagation by means of two electromagnetic solvers, namely: (i) plaSma Padova Inhomogeneous Radial Electromagnetic solver (SPIREs), a mono-dimensional finite-difference frequency-domain code, and (ii) Advanced coDe for Anisotropic Media and ANTennas (ADAMANT), a full-wave three-dimensional tool based on the method of moments. We have computed the deposited power spectrum with SPIREs, power deposition profile with ADAMANT and the antenna impedance with both codes. First we have verified the numerical accuracy of both SPIREs and ADAMNT. Then, we have analysed two configurations of magnetostatic field, namely produced by Maxwell coils, and Helmholtz coils. For each configuration we have studied three cases: (i) low density $n=10^{17}~\text{m}^{-3}$ and low magnetic field $B_{0}=250$  G; (ii) medium density $n=10^{18}~\text{m}^{-3}$ and medium magnetic field $B_{0}=500$  G; (iii) high density $n=10^{19}~\text{m}^{-3}$ and high magnetic field $B_{0}=1000$  G. We have found that the Maxwell coil configuration does not produces significant changes in the deposited power phenomenon with respect to a perfectly uniform and axial magnetostatic field. While the Helmholtz coil configuration can lead to a power spectrum peaked near the axis of the discharge.


2020 ◽  
Vol 29 (8) ◽  
pp. 085007
Author(s):  
Anshu Verma ◽  
A Ganguli ◽  
D Sahu ◽  
Ramesh Narayanan ◽  
R D Tarey

2001 ◽  
Vol 390 (1-2) ◽  
pp. 107-112 ◽  
Author(s):  
Jun Xu ◽  
Xinlu Deng ◽  
Jialiang Zhang ◽  
Wenqi Lu ◽  
Tengcai Ma

2004 ◽  
Vol 151 (10) ◽  
pp. C649 ◽  
Author(s):  
Gratiela I. Isai ◽  
Jisk Holleman ◽  
Hans Wallinga ◽  
Pierre H. Woerlee

1996 ◽  
Vol 423 ◽  
Author(s):  
Y. C. Kao ◽  
T. P. E. Broekaert ◽  
H. Y. Liu ◽  
S. Tang ◽  
I. H. Ho ◽  
...  

AbstractIn this paper, we report the MBE growth of high nitrogen content lattice-matched InAs1−xNx (x=0.38) single crystal epitaxial films on GaAs. The nitrogen incorporation is about an order higher than previously reported on other mixed group V nitride alloys. These data are consistent with a nitrogen solubility limit calculation in various III-V binary alloys, which predicts orders of magnitude higher nitrogen incorporation in InAs than any other alloys. InAsN growths were obtained using a modified ECR-MBE system with atomic-nitrogen generated by an ECR plasma source. Improved crystal quality was obtained using a “template” growth technique. An x-ray linewidth of 270 arc-s was achieved on a 0.4 μm thick InAs0.62N0.38/GaAs multi-layer structure. Hall effect data show these InAsN films are semi-metallic.


2002 ◽  
Vol 11 (4) ◽  
pp. 361-367 ◽  
Author(s):  
M Naddaf ◽  
V N Bhoraskar ◽  
A B Mandale ◽  
S R Sainkar ◽  
S V Bhoraskar

Sign in / Sign up

Export Citation Format

Share Document