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Oxidation and wet etching behavior of sputtered Mo-Ti-Al filmsTanja Jörg, Anna M. Hofer, Harald Köstenbauer, Jörg Winkler, and Christian Mitterer
Citation: Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 36, 021513 (2018);View online: https://doi.org/10.1116/1.5009289View Table of Contents: http://avs.scitation.org/toc/jva/36/2Published by the American Vacuum Society
Oxidation and wet etching behavior of sputtered Mo-Ti-Al films
Tanja J€orga) and Anna M. HoferDepartment of Physical Metallurgy and Materials Testing, Montanuniversit€at Leoben, Franz-Josef-Straße 18,8700 Leoben, Austria
Harald K€ostenbauer and J€org WinklerBusiness Unit Coating, PLANSEE SE, Metallwerk-Plansee-Straße 71, 6600 Reutte, Austria
Christian MittererDepartment of Physical Metallurgy and Materials Testing, Montanuniversit€at Leoben, Franz-Josef-Straße 18,8700 Leoben, Austria
(Received 14 October 2017; accepted 9 January 2018; published 24 January 2018)
Exposure of Mo thin films above 300 �C in ambient atmosphere results in surface oxidation,
leading to the formation of colored oxide films deteriorating their performance in thin film
transistor liquid crystal displays. In this study, the influence of the alloying elements Ti and Al
on microstructure, electrical properties, oxidation and wet etching behavior of Mo thin films
was investigated. Mo1�x�yTixAly films (with x� 0.08 and 0� y� 0.24) were deposited by direct
current magnetron sputtering and annealed in ambient air at 330 �C for 1 h. The oxidation
resistance of Mo-Ti-Al films was enhanced with increasing Al content. A minimum Al content of
y¼ 0.16 was necessary to form a thin protective Al2O3 surface layer and to prevent the formation
of colored molybdenum oxides. The wet etching rate of the Mo-Ti-Al films in a commonly used
mixture of phosphoric-, acetic-, and nitric acid decreased with increasing Al content, but was still
acceptable for thin film transistor liquid crystal displays applications. Published by the AVS.https://doi.org/10.1116/1.5009289
I. INTRODUCTION
Sputtered Mo thin films are used in thin film transistor
liquid crystal displays (TFT-LCD) as conducting materials.
Their low electrical resistance and easy chemical patterning
make them an excellent material for gate, source/drain elec-
trodes and signal and data bus-lines.1,2 In addition, Mo thin
films serve as bottom and capping layers in the gate metalli-
zation of TFTs, due to their good adhesion on glass and low
contact resistance to silicon and indium tin oxide.3,4 They
are also utilized as diffusion barrier layer between Cu and Si
in the Cu process, based on their high melting point and very
low diffusion coefficients.5,6 Since annealing treatments are
used in TFT-LCD processing,7 these films have to withstand
thermal exposure without deterioration of their properties.
However, Mo is known to exhibit poor oxidation resistance
in air and is prone to oxidation above 300 �C.8,9 Previous
studies on binary Mo alloys indicated that alloying can be
used to improve the oxidation resistance.10 For example,
Park et al. have reported that Ti is corrosion resistant in oxi-
dizing atmospheres, and that alloying of Ti to Mo leads to
the formation of a passivation layer.11 However, Ti cannot
be dissolved in phosphoric, acetic, nitric acid solutions
(PAN),12 which is a key process step in the production of
TFT materials. In contrast to Ti, Al is known for its superior
oxidation resistance and at the same time its good wet etch-
ing behavior in PAN.12 Thus, the aim of the present work is
to synthesize ternary Mo-Ti-Al thin film alloys by magne-
tron sputter deposition and to study their oxidation resistance
and wet etching ability for varying Al contents.
II. EXPERIMENTAL DETAILS
The films were grown in a laboratory-scale unbalanced
direct current (dc) magnetron sputter system, using one
Mo0.9Ti0.1 (atomic fractions) and one Al target (150.8 mm� 6 mm), which were mounted on two unbalanced
magnetrons (AJA International, Inc.). The substrate material,
boron-silicate glass (Corning EAGLE2000TM AMLCD,
size 50� 50 mm2), and Si (100) were ultrasonically cleaned
in a commercial detergent from Borer Chemie AG or etha-
nol, respectively, and fixed on a rotatable sample holder
positioned about 55 mm above the magnetrons. After reach-
ing a base pressure of less than 2� 10�3 Pa, plasma etching
of the substrates was performed by applying a pulsed dc dis-
charge of �500 V and 250 kHz at an Ar gas pressure of 1 Pa
for 2 min. Depositions were carried out at an Ar pressure of
0.4 Pa, while no intentional substrate heating was used.
Different Al contents within the films were obtained by vary-
ing the dc current on the Al target between 0 and 0.15 A,
whereas the current on the Mo0.9Ti0.1 target was held con-
stant at 0.35 A. Depending on the Al current, the growth rate
varied from 31 to 42 nm/min; hence, the deposition time was
adjusted to obtain a film thickness of �250 nm for all films.
Film thickness measurements were performed by investi-
gating the fracture cross-sections of the films grown on Si
with a scanning electron microscope (SEM, Zeiss Evo-50).
The chemical composition of the films on Si was evaluated
using energy-dispersive X-ray spectroscopy (EDX) with an
Oxford Instruments INCA extension attached to the SEM.
All further investigations were conducted on the films grown
on boron-silicate glass. The crystallographic structure was
characterized by X-ray diffraction (XRD) in h/2h geometrya)Electronic mail: [email protected]
021513-1 J. Vac. Sci. Technol. A 36(2), Mar/Apr 2018 0734-2101/2018/36(2)/021513/5/$30.00 Published by the AVS. 021513-1
using a Bruker-AXS D8 Advance diffractometer equipped
with Cu-Ka radiation and parallel beam optics. The wet etch-
ing rate of the as-deposited films was determined by the
weight difference of the films before and after dipping into
the etchant. The etching solution (PAN) was composed of
66% phosphoric acid, 10% acetic acid and 5% nitric acid by
weight. All wet etching tests were carried out at a stirring
rate of 300 rpm at 40 �C. To evaluate the oxidation behavior
of the films, the as-deposited samples were annealed in a
chamber furnace in air at 330 �C for 1 h. The electrical sheet
resistivity and reflectance UV-Vis spectra of the films were
determined prior and after the annealing step with a Jandel
RM2 four-point probe and a Perkin Elmer Lambda 950
photo-spectrometer, respectively. The Raman spectra of the
annealed films were obtained using a Jobin Yvon LabRam
confocal Raman spectrometer employing a Nd:YAG laser
(k¼ 532 nm, 10 mW). The oxidation states of the films after
annealing were studied by X-ray photoelectron spectroscopy
(XPS) using an Omicron Multiprobe system with a mono-
chromized Al Ka beam (1486.6 eV) and a resolution <0.5 eV.
In order to remove the volatile surface contaminants, the
samples were heated for 20 min at 300 �C before XPS
measurements.
III. RESULTS AND DISCUSSION
Figure 1 illustrates the X-ray diffractograms of all
Mo1�x�yTixAly films in the as-deposited state (x and y in at.
% determined by EDX). It should be noted that the ratio of
Ti:Al in the films almost linearly increases from 1:1 via 1:2
to 1:3 with a corresponding decrease of the Mo content. The
diffraction patterns reveal the formation of a single-phase
body-centered cubic Mo-based solid solution (space group
Im-3m, ICDD 03-065-7442) for all films synthesized. While
(110)-oriented crystallites dominate for all compositions
studied, diffraction of (100)-oriented crystallites enhances
with increasing Al content. The results are consistent with a
previous study by Lorenz et al.,13 who investigated Mo-Al
thin films containing up to 32 at. % Al.
The evolution of the wet etching rate in PAN of the unal-
loyed Mo and Mo1�x�yTixAly films with increasing Al con-
tent is displayed in Fig. 2. It can be seen that for adding
approximately 8 at. % Ti to Mo only slightly decreases the
dissolution rate by 7.4%. For comparison, the wet etching
rate of a Mo-Ti film containing 18 at. % Ti was determined
208 6 2 nm/min. This substantial reduction of the wet etch-
ing rate is attributed to the insolubility of Ti in PAN.12 In
contrast, Al has a higher solubility than Ti, but the incorpora-
tion of Al in Mo still gradually decreases the wet etching
rate with increasing Al content. This is in good agreement to
Kim et al.,14 who reported that Mo exhibits a higher wet
etching rate than Al in PAN and that the contact of the less
noble Al decreases the dissolution rate of the nobler Mo.
Annealing tests in air at 330 �C were performed to investi-
gate the oxidation resistance of the alloyed films compared to
the pure Mo film. It is evident, that the Al content significantly
influences the oxidation behavior of the films. The pure Mo
film [see Fig. 3(a)] exhibits poor resistance to oxidation at
330 �C, leading to the formation of a colored oxide film. A
similar behavior can be observed for the Mo0.92Ti0.08 and
Mo0.92Ti0.08Al0.08 films. However, the ternary Mo1�x�yTixAlyfilms with y> 0.08 [Figs. 3(d)–3(e)] remain colorless after the
heat treatment, retaining their initial mirrorlike appearance,
indicating the formation of a very thin transparent protective
oxide film.
The influence of the annealing treatment on the electrical
resistivity is plotted in Fig. 4 as a function of the Al content.
A pure Mo film (300 nm thick), as reported in our earlier
work,15 has a resistivity of about 10 lX cm. Alloying 8 at.%
Al to the Mo0.92Ti0.08 solid solution causes a sharp rise of
electrical resistivity to approximately 100 lX cm. However,
further Al additions result in a linear increase of the resistiv-
ity. This behavior is in good agreement with the develop-
ment of resistivity against alloying content of solid solutions
and can be explained by the different atom size of the alloy-
ing elements, which lead to an increase of electron scatter-
ing. Furthermore, alloying elements introduce local charge
differences, due to their different valence electrons, which
FIG. 1. (Color online) X-ray diffractograms of as-deposited Mo1�x�yTixAlyfilms.
FIG. 2. (Color online) Wet etching rate in PAN for Mo1�x�yTixAly films
(with x� 0.08 and 0� y� 0.24) plotted over the Al content. Open symbol
denotes the etching rate of the unalloyed Mo film.
021513-2 J€org et al.: Oxidation and wet etching behavior of sputtered Mo-Ti-Al films 021513-2
J. Vac. Sci. Technol. A, Vol. 36, No. 2, Mar/Apr 2018
results in a higher electron scattering probability.16 The
obtained resistivity values are comparable to those found for
Mo-Al alloys13 and are considered acceptable for TFT-LCD
applications.17 No significant difference between the electri-
cal resistivity before and after annealing is observed. While
annealing could be expected to slightly reduce the electrical
resistivity due to annihilation of point defects,18 the forma-
tion of oxide films—assuming that the oxide films are not
destroyed during four-point probe measurement—might
compensated for the defect annihilation.
The reflectance spectra of the Mo0.84Ti0.08Al0.08 and
Mo0.76Ti0.08Al0.16 films in the as-deposited and annealed
state are presented in Fig. 5. Both films show in the as-
deposited state an average reflectance of above 50%, con-
firming the metallic appearance. Moreover, the Al fraction
in the films has a strong influence on the optical properties
of the annealed samples. The reflectance of the Mo film con-
taining 8 at. % Al decreases significantly after annealing and
shows an absorption edge below 400 nm. The strong absorp-
tion in the violet region of the spectrum is responsible for
the yellowish color of the film [see Fig. 3(c)] and indicates
the formation of an oxide layer. However, by increasing
the Al content to 16 at. %, the decrease in reflectivity after
annealing is reduced and the formation of the absorption
edge is prevented. As a result, the optical appearance
remains metallic [Fig. 3(d)].
The oxide films formed during annealing are too thin to
be detected by XRD and in SEM cross-sections. To obtain
more information about the surface oxides, which are
responsible for the thermal coloration of the films, Raman
spectroscopy was performed. Molybdenum oxides are well
suited for characterization by Raman scattering.19 In contrast,
annealing of bulk Al below 350 �C leads to the formation of
an amorphous Al2O3 film,20 which cannot be detected by
Raman spectroscopy.21,22 Figure 6 shows the Raman spectra
of the annealed samples, which are in good agreement with
the results of visual inspection and spectroscopy. The Raman
spectrum of the reference Mo film is characteristic for poly-
crystalline MoO3 bands (995, 818 and 665 cm�1). Thus, the
annealing treatment causes surface oxidation of the unalloyed
Mo film, leading to the formation of MoO3. The Raman spec-
tra of the Mo0.84Ti0.08 and Mo0.84Ti0.08Al0.08 film are nearly
identical. Both indicate broadening of the peaks, suggesting
the presence of mixed oxides.23 In contrast, no Raman peaks
are observable for the ternary Mo1�x�yTixAly films with
y> 0.08, indicating the absence of the Raman-active MoO3
and TiO2. Therefore, it can be concluded that an increased Al
FIG. 3. (Color online) Photographs of the investigated films after annealing at 330 �C for 1 h in air.
FIG. 4. (Color online) Electrical resistivity of the Mo1�x�yTixAly films (with
x� 0.08 and 0� y� 0.24) vs the Al content in the as-deposited and
annealed state. The electrical resistivity of a 300 nm thick Mo film reported
in our earlier work (Ref. 15) is given as a reference.
FIG. 5. (Color online) Optical reflectance spectra before and after annealing
of (a) Mo0.84Ti0.08Al0.08 and (b) Mo0.76Ti0.08Al0.16.
021513-3 J€org et al.: Oxidation and wet etching behavior of sputtered Mo-Ti-Al films 021513-3
JVST A - Vacuum, Surfaces, and Films
content prevents the formation of MoO3 and results in growth
of a protective Al2O3 film.
In order to study the influence of Al on the oxidation
states of Mo and to verify the presence of the assumed
Al2O3 film, XPS analyses were conducted. As a result of
spin-orbit (j-j) coupling, the Mo3d spectrum consists of the
characteristic Mo3d5/2-Mo3d3/2 doublet.24 Figure 7 repre-
sents the Mo3d XPS spectra of the Mo-Ti-Al films with dif-
ferent Al contents. Again, the spectra of the Mo0.84Ti0.08 and
Mo0.84Ti0.08Al0.08 films exhibit substantial similarity. Curve
fitting of the Mo3d5/2 peak indicates two spectral lines at
231.8 and 232.7 eV, which are assigned to Mo5þ and Mo6þ
states. These peak positions agree well with earlier reports.25
Clearly, the intensity of the Mo6þ oxidation state exceeds
the one of the Mo5þ oxidation state and is the major contribu-
tion to the Mo3d5/2 signal of the MoTi8 and MoTi8Al8 films.
Hence, annealing of the low-alloyed films in air is enhancing
the Mo6þ state, evidencing the formation of MoO3. However,
the XPS spectra of the ternary Mo1�x�yTixAly films with
y> 0.08 alter with increasing Al content. For y¼ 0.16 several
oxidation states can be identified, with binding energies of the
Mo3d5/2 corresponding to metallic Mo0 (227.9 eV), Mo4þ
(229.1 eV), Mo5þ (232.0 eV) and Mo6þ (233.1 eV). Similar
findings have also been reported by Kim et al.26 As the Al
content is further increased (y¼ 0.24), the same oxidation
states and one additional species of Mo is observed, with a
binding energy of 228.3 eV. Since the binding energy of this
oxidation state is between Mo4þ and the metallic Mo0, it is
referred to as Modþ. Choi and Thompson assigned this Mo
species to Mo3þ, Xiang et al. to Mo2þ.24,27 Increasing the Al
content decreases the intensity of the Mo6þ peaks and favors
reduced oxidation states of Mo. Accordingly, the intensity
of the metallic Mo0 peak is the highest observed in the
Mo0.69Ti0.07Al0.24 film (see Fig. 7).
The results of peak area analysis of the Ti2p and Al2p
bands are summarized in Table I. It shows that an increasing
Al content leads to enhanced formation of Al2O3. As a conse-
quence, it can be presumed that the formation of Al2O3 is
responsible for the reduced oxidation states of Mo. Therefore,
the oxidation behavior of Mo-Ti-Al films is primarily con-
trolled by the Al content in the films. This conclusion is in
agreement to a study by Kai et al.28 on the oxidation of a Zr-
Cu-Al-Ni amorphous alloy in air at 300–425 �C.
IV. CONCLUSIONS
The influence of different Al contents on phase evolution,
wet etching behavior and oxidation resistance of Mo-Ti-Al
films deposited by dc magnetron sputtering was investigated.
All films show a single-phase body-centered cubic structure
based on the Mo phase. An increasing Al content results in a
decline of the wet etching behavior of the Mo alloy films in a
66 wt. % phosphoric acid, 10 wt. % acetic acid and 5 wt. %
nitric acid (PAN), but is still in an acceptable range for thin
film transistor liquid crystal display applications. The forma-
tion of MoO3 during the annealing at 330 �C for 1 h is respon-
sible for the thermal coloration of the unalloyed Mo and the
low-alloyed Mo0.84Ti0.08 and Mo0.84Ti0.08Al0.08 films. The
further increasing Al content promotes the formation of an
amorphous Al2O3 layer, which reduces the oxidation states of
Mo. Thus, the oxidation behavior of Mo1�x�yTixAly films is
primarily controlled by the Al content, where a minimum
alloying element content of x¼ 0.08 and y� 0.16 was found
to be necessary to enhance the oxidation resistance at still
acceptable wet etching rates.
ACKNOWLEDGMENTS
Funding for this research has been provided by the€Osterreichische Forschungsf€orderungsgesellschaft mbH within
the framework of the Headquarters project E2SPUTTERTECH
(Project No. 841482). The authors are grateful to Alexander
FIG. 6. (Color online) Raman spectra of the Mo1�x�yTixAly films compared
to a Mo reference after annealing at 330 �C for 1 h in air.
FIG. 7. (Color online) Mo3d XPS spectra of the Mo1�x�yTixAly films after
annealing at 330 �C for 1 h in air.
TABLE I. Results of quantitative peak area analysis of the Ti2p and Al2p
XPS bands.
Atomic fraction (%)
Ti
(453.9 eV)
TiO2
(458.9 eV)
Al
(72.3 eV)
Al2O3
(74 eV)
Mo0.92Ti0.08 — 2.51 — —
Mo0.84Ti0.08Al0.08 — 2.61 — 3.58
Mo0.76Ti0.08Al0.16 — 2.59 0.18 7.18
Mo0.69Ti0.07Al0.24 0.15 2.45 1.59 11.29
021513-4 J€org et al.: Oxidation and wet etching behavior of sputtered Mo-Ti-Al films 021513-4
J. Vac. Sci. Technol. A, Vol. 36, No. 2, Mar/Apr 2018
Fian (Joanneum Research, Weiz, Austria) for XPS
measurements and to Ronald Bakker (Montanuniversit€at
Leoben) for the assistance with Raman spectroscopy. Gerhard
Hawranek (Montanuniversit€at Leoben) is thanked for SEM
characterization.
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