The remote plasma deposition of hydrogenated amorphous carbon (a-C:H) thin films is investigated by in situ spectroscopic ellipsometry (SE). The dielectric function of the a-C:H film is in this paper parametrized by means of B-splines. In contrast with the commonly used Tauc–Lorentz oscillator, B-splines are a purely mathematical description of the dielectric function. We will show that the B-spline parametrization, which requires no prior knowledge about the film or its interaction with light, is a fast and simple-to-apply method that accurately determines thickness, surface roughness, and the dielectric constants of hydrogenated amorphous carbon thin films. Analysis of the deposition process provides us with information about the high deposition rate, the nucleation stage, and the homogeneity in depth of the deposited film. Finally, we show that the B-spline parametrization can serve as a stepping stone to physics-based models, such as the Tauc–Lorentz oscillator.

1.
J. W. A. M.
Gielen
,
W. M. M.
Kessels
,
M. C. M.
van de Sanden
, and
D. C.
Schram
,
J. Appl. Phys.
82
,
2643
(
1997
).
2.
J.
Robertson
,
Mater. Sci. Eng., R.
37
,
129
(
2002
).
3.
J.
Benedikt
,
K. G. Y.
Letourneur
,
M.
Wisse
,
D. C.
Schram
, and
M. C. M.
van de Sanden
,
Diamond Relat. Mater.
11
,
989
(
2002
).
4.
S. V.
Singh
,
M.
Creatore
,
R.
Groenen
,
K.
Van Hege
, and
M. C. M.
van de Sanden
,
Appl. Phys. Lett.
92
,
221502
(
2008
).
5.
H.
Fujiwara
,
Spectroscopic Ellipsometry: Principles and Applications
(
John Wiley & Sons Ltd.
,
Chichester, UK
,
2007
).
6.
Handbook of Ellipsometry
, edited by
H. G.
Thompkins
and
E.
Irene
(
William Andrew Inc.
,
Norwich, New York
,
2005
).
7.
E.
Langereis
,
S. B. S.
Heil
,
H. C. M.
Knoops
,
W.
Keuning
,
M. C. M.
van de Sanden
, and
W. M. M.
Kessels
,
J. Phys. D
42
,
073001
(
2009
).
8.
S.
Kassavetis
,
P.
Patsalas
,
S.
Logothetidis
,
J.
Robertson
, and
S.
Kennou
,
Diamond Relat. Mater.
16
,
1813
(
2007
).
9.
S.
Logothetidis
,
Diamond Relat. Mater.
12
,
141
(
2003
).
10.
S. S.
Zumdahl
,
Chemical Principles
, 3rd ed. (
Houghton Mifflin
,
Boston, MA
,
1998
).
11.
G. E.
Jellison
and
F. A.
Modine
,
Appl. Phys. Lett.
69
,
371
(
1996
).
12.
J.
Fink
,
T.
Müller-Heinzerling
,
J.
Pflüger
,
B.
Scheerer
,
B.
Dischler
,
P.
Koidl
,
A.
Bubenzer
, and
R.
Sah
,
Phys. Rev. B
30
,
4713
(
1984
).
13.
S.
Waidmann
,
M.
Knupfer
,
J.
Fink
,
B.
Kleinsorge
, and
J.
Robertson
,
J. Appl. Phys.
89
,
3783
(
2001
).
14.
B.
Johs
and
J. S.
Hale
,
Phys. Status Solidi A
205
,
715
(
2008
).
15.
16.
A.
von Keudell
and
W.
Jacob
,
J. Appl. Phys.
79
,
1092
(
1996
).
17.
M. C. M.
van de Sanden
,
G. M.
Janssen
,
J. M.
de Regt
,
D. C.
Schram
,
J. A. M.
van der Mullen
, and
B.
van der Sijde
,
Rev. Sci. Instrum.
63
,
3369
(
1992
).
18.
G. M. W.
Kroesen
,
D. C.
Schram
, and
J. C. M.
de Haas
,
Plasma Chem. Plasma Process.
10
,
531
(
1990
).
19.
J. W. A. M.
Gielen
,
M. C. M.
van de Sanden
,
P. R. M.
Kleuskens
, and
D. C.
Schram
,
Plasma Sources Sci. Technol.
5
,
492
(
1996
).
20.
J. A. Woollam Co, Inc.
, personal communication 6 July (
2009
).
21.
A change in one of the ci coefficients affects the next four segments, as can be seen from the recursive formula.
22.
J. A. Woollam Co., Inc.
, CompleteEASE TM software manual, version 3.18 ed. (
2007
).
23.
I. -Y.
Kim
,
S. -H.
Hong
,
A.
Consoli
,
J.
Benedikt
, and
A.
von Keudell
,
J. Appl. Phys.
100
,
053302
(
2006
).
24.
N.
Savvides
,
J. Appl. Phys.
59
,
4133
(
1986
).
25.
J. W. A. M.
Gielen
,
M. C. M.
van de Sanden
, and
D.
Schram
,
Appl. Phys. Lett.
69
,
152
(
1996
).
26.
J. W. A. M.
Gielen
,
P. R. M.
Kleuskens
,
M. C. M.
van de Sanden
,
L. J.
van Ijzendoorn
,
D. C.
Schram
,
E. H. A.
Dekempeneer
, and
J.
Meneve
,
J. Appl. Phys.
80
,
5986
(
1996
).
You do not currently have access to this content.