April 30, 2010 / Vol. 8, Supplement / CHINESE OPTICS LETTERS 73
Characterization of metal-oxide thin films deposited by
plasma-assisted reactive magnetron sputtering
Stefan Jakobs
1∗
, Marc Lappschies
1
, Uwe Schallenberg
1
, Olaf Stenzel
2
, and Steffen Wilbrandt
2
1
Mso Jena GmbH, Carl-Zeiss-Promenade 10, 07745 Jena, Germany
2
Fraunhofer IOF, Alb ert-Einstein-Straße 7, 07745 Jena, Germany
∗
E-mail: jakobs@mso-jena.de
Received Octob er 30, 2009
For single layers of SiO
2
, Nb
2
O
5
, and Ta
2
O
5
that are deposited by plasma-assisted reactive magnetron
sputtering (PARMS), we present measurement results for basic optical and mechanical prop erties, in
particular, optical index, intrinsic film stress, thermal shift of spectral transmittance, and microroughness.
We find high refractive indices combined with low intrinsic film roughness, moderate compressive stress, and
almost a vanishing shift, indicate high potential for the production of high-performance optical coatings.
The high thickness accuracy and process stability are exemplified by the measured spectral performance
of multilayer stacks with ab out 200 single layers.
OCIS co des: 310.1860, 310.6860.
doi: 10.3788/COL201008S1.0073.
Plasma-assisted reactive magnetron sputtering (PARMS)
is a new technique for deposition of high-quality optical
coatings. It has been developed to achieve process re-
producibility and film thickness accuracy typical of ion-
beam sputtering. Deposition rates are retained at the
same range as in electron beam evaporation processes.
This study aims to characterize basic material proper-
ties of SiO
2
, Nb
2
O
5
, and Ta
2
O
5
deposited by PARMS,
in particular, optical index in ultraviolet (UV)/visible
(Vis)/near-infrared (NIR) area, intrinsic film stress, ther-
mal shift of spectral transmittance, and microroughness.
Each of these properties may be crucial for the suitability
of a deposition technique for a specific field of applica-
tion. We compare the results for the layers deposited
by PARMS with those deposited by plasma ion-assisted
deposition (PIAD), as well as with results of a recent
study
[1]
on optical and mechanical properties of oxide
optical coating materials deposited by a variety of state-
of-the-art thin-film deposition techniques.
In addition, we present examples of complex optical
coatings deposited by PARMS to demonstrate the poten-
tial of the technique in high-performance applications.
Our investigation was focused on the properties of
metal-oxide films deposited by PARMS (Leybold HE-
LIOS sputter system). SiO
2
, as a low-index material,
and Ta
2
O
5
or Nb
2
O
5
, as high-index materials, were sput-
tered by two dual magnetrons from metal targets. An RF
plasma source was used to assist complete oxidation of
the thin film materials. Substrates were placed onto a
load lock on a horizontally rotating turntable. Optical
monitoring was used for in situ measurement of optical
film thickness and process control. Deposition rates var-
ied in dependence vis-`a-vis particular layer thicknesses.
The average rate for deposition of a multilayer stack was
about 0.4 nm/s or 1.5 µm/h.
For comparison, we deposited single layers of SiO
2
and Ta
2
O
5
by electron beam evaporation with ion as-
sistance (Leybold Advanced Plasma Source)
[2]
. During
film growth on the substrate, the film material was bom-
barded by argon ions with energies of about 120 eV.
Deposition rates were 0.5 and 0.35 nm/s for SiO
2
and
Ta
2
O
5
, respectively.
All layers and layer systems were dep osited at mso jena
onto polished fused silica and BK7 glass substrates at a
diameter of 25 mm and thickness of 3 mm; for stress mea-
surements, onto Si wafer at a diameter of 76.2 mm with
thickness of 0.38 mm.
Spectrophotometry (Perkin Elmer Lambda 900 scan-
ning spectrophotometer) was used to determine optical
constants at Fraunhofer IOF. Transmittance (T ) and re-
flectance (R) were measured at nearly normal incidence
using a self-developed VN attachment, particularly, for
absolute reflectance measurements. From these sp ectra,
optical constants n (refractive index) and k (extinction
coefficient) were deduced from spectra fits in terms of a
Lorentzian multi-oscillator model
[3]
. The accuracy in n-
determination was of the order of 1% relative error. From
the same spectra fits, the thickness of the layers was also
determined.
The thermal shift of the same samples was determined
Table 1. Overview of Samples for Measured
Thickness Determined by Spectrophotometry
Process
Material Type
Target Measured
/Process ID
Thickness Thickness
(nm) (nm)
PARMS
H0058 SiO
2
single layer 370 369.5
H0061 SiO
2
single layer 2000 2019
H0057 Ta
2
O
5
single layer 250 251.7
H0062 Ta
2
O
5
single layer 2000 2012
H0066 Nb
2
O
5
single layer 230 230.2
H0067 Nb
2
O
5
single layer 2000 2002
H0074 SiO
2
/Ta
2
O
5
notch filter 19757
405/488/561/639
H0078 SiO
2
/Nb
2
O
5
band pass 15400
420–480
PIAD
U651 Ta
2
O
5
single layer 2000 1949
U653 SiO
2
single layer 2000 1962
1671-7694/2010/S10073-05
c
° 2010 Chinese Optics Letters