Herein, TiO2 coatings were deposited on photodegradable polymers for protection from UV irradiation using the atmospheric-pressure plasma-enhanced chemical vapor deposition (AP-PECVD) technique. Polymethylmethacrylate (PMMA) and polycarbonate (PC) substrates were coated with titanium tetraisopropoxide as the precursor in an open-air atmospheric-pressure nonequilibrium argon plasma jet. The AP-PECVD-derived TiO2 coatings exhibited good adhesion to PMMA and PC. The TiO2 coatings could shield more than 99% of UV light in the wavelength range of 200-300 nm, without affecting the transmittance of visible light. UV irradiation tests on polymer films demonstrated that the degradation rates of PMMA and PC were significantly reduced by one-tenth after they were coated with TiO2 films.
Herein, TiO2 coatings were deposited on photodegradable polymers for protection from UV irradiation using the atmospheric-pressure plasma-enhanced chemical vapor deposition (AP-PECVD) technique. Polymethylmethacrylate (PMMA) and polycarbonate (PC) substrates were coated with titanium tetraisopropoxide as the precursor in an open-air atmospheric-pressure nonequilibrium argon plasma jet. The AP-PECVD-derived TiO2 coatings exhibited good adhesion to PMMA and PC. The TiO2 coatings could shield more than 99% of UV light in the wavelength range of 200-300 nm, without affecting the transmittance of visible light. UV irradiation tests on polymer films demonstrated that the degradation rates of PMMA and PC were significantly reduced by one-tenth after they were coated with TiO2 films.
Transparent
plastics, such as polymethylmethacrylate (PMMA) and
polycarbonate (PC), are being used to replace glass for both industrial
and domestic purposes. However, long-term exposure of PMMA and PC
to UV irradiation causes severe degradation of these polymers due
to UV-induced photochemical oxidation.[1] Although PMMA and PC have outstanding optical clarity and mechanical
properties, their photosensitive nature renders them unsuitable for
application in outdoor conditions, for example, car windows, greenhouse,
and electronics. Hence, transparent UV-protective coatings are required
to protect these polymers. Aklalouch et al. successfully covered PMMA
sheets with a hybrid organic–inorganic sol–gel coating
that comprised organically modified silicate and CeO2 nanoparticles.
This hybrid coating showed efficient UV protection in the outdoor
weathering aging test for the application of concentrated photovoltaic
panels.[2] Anma et al. coated ZnO thin films
on PC plates via the plasma-enhanced chemical vapor deposition (PECVD)
method. The obtained ZnO-coated PC was observed to exhibit outstanding
characteristics of UV protection in the xenon arc weatherability test,
wherein it remained smooth and uncolored even after 1000 h of UV irradiation.[3] Weber et al. fabricated vacuum-deposited organic–inorganic
hybrid coatings embedded with hydroxyphenyltriazine and hydroxybenzotriazoles
for UV protection of PC. The fabricated hybrid coatings exhibited
high stability during UV irradiation experiments.[4]Currently, there are several UV absorbers available
for UV protection,
including titanium dioxide (TiO2),[5] cerium oxide,[6] zinc oxide,[7] 2,2-dihydroxy-4-methoxy-benzophenone,[8] MIL-125(Ti)-NH2, and MIL-68(In)-NH2.[9] TiO2 is one of the
most widely used UV absorbers because it exhibits nontoxicity, good
physical and chemical stabilities, cost effectiveness, good visible
light transparency, and outstanding UV-blocking properties.[10−12] TiO2 has also been used as a UV-protective coating on
polymers. Cui et al. studied the coating of a transparent TiO2/mixed oxide UV-protective thin film on heat-sensitive substrates
using a low-temperature sol–gel method.[13] Hwang et al. also fabricated a TiO2 UV-protective
hard coating and deposited it via spray coating on PC.[14] However, the use of solvents in the aforementioned
methods renders the fabrication process complex and leads to a waste
of chemicals.Atmospheric-pressure plasma-enhanced chemical
vapor deposition
(AP-PECVD) is a single-step solvent-free technique,[15,16] which has recently drawn considerable attention for the fabrication
of oxide coatings on polymers. Unlike the low-pressure plasma-enhanced
chemical vapor deposition, AP-PECVD can be operated without a vacuum
system; this eliminates the required limits with regard to the shape
and size of the coated materials.[17,18] Moreover,
the use of plasma has enabled fabrication at low temperatures, wherein
the film formation reaction proceeds by the collision of monomers
with charged particles (electrons, ions) in the plasma and not by
thermal decomposition.[19,20] Therefore, the low processing
temperature of AP-PECVD can prevent the polymers from melting. In
addition, an improvement in the adhesion of oxide coatings to polymers
using AP-PECVD is possible owing to the surface modification of the
polymer using plasma in the initial stage of deposition.[21] Scopece et al. studied the deposition of SiO on polypropylene for gas permeation by an atmospheric-pressure
plasma jet using hexamethyldisiloxane as the precursor.[22] Watanabe et al. showed that ZnO transparent
thin films can be deposited onto polymer substrates by atmospheric
plasma in ambient air at room temperature using diethylzinc as the
precursor.[23] Therefore, comparing with
the reported UV-protective film coating methods, including hydrothermal
method and sol–gel method, the AP-PECVD technique could overcome
the drawbacks like a complex process, high processing temperature,
and use of a solvent due to its single-step, solvent-free, low-temperature,
and vacuum-free fabrication process.In our previous studies,[24,25] we successfully applied
AP-PECVD for the fabrication of TiO2 thin films at room
temperature, which can exclude the use of solvents during fabrication
as compared to the sol–gel method and the spray coating technique.
Furthermore, we described the film formation mechanism that was dependent
on the process parameters. We reported that the morphologies of the
films, which determine their optical properties, are extremely sensitive
to the deposition temperature and precursor concentration. Moreover,
we demonstrated that TiO2 films fabricated at optimized
conditions demonstrate an excellent absorption of UV light and visible
light transparency. Accordingly, AP-PECVD has proven to have potential
advantages for the fabrication of TiO2 coatings onto polymers,
which can improve the stability of polymers against UV irradiation.
However, our previous studies were primarily performed using silicon
and glass as the substrates; this was done to ensure that the substrate
is stable under plasma exposure and the film formation mechanism could
be properly discussed. To our knowledge, there are limited reports
on the fabrication of TiO2 coatings on polymers via AP-PECVD,
and hence the effect of AP-PECVD-derived TiO2 coatings
on the improvement of the stability of polymers against UV irradiation
has merely been reported.In the present work, therefore, we
investigated AP-PECVD of TiO2 coatings onto transparent
plastics and their capability to
prevent the UV-induced photodegradation of polymers. In the first
part of the present work, we performed the deposition of TiO2 coatings using PMMA and
PC as the polymer substrates. The UV-shielding properties of the TiO2 coatings were investigated using ultraviolet–visible
(UV–vis) spectroscopy. We also confirmed that the structures
of the polymer substrates were unchanged after AP-PECVD, and that
the obtained TiO2 coatings had high adhesion, proving that
AP-PECVD of TiO2 is applicable for the polymer substrates.
Subsequently, in the second part of the present work, we demonstrated
the UV-absorbing capability of TiO2 coatings formed on
the polymer substrates and revealed their ability to prevent the UV-induced
photodegradation of polymer substrates. To this end, we conducted
UV-irradiation tests on the polymer films with and without TiO2 coatings and tracked the change in Fourier transform infrared
(FTIR) spectra with UV irradiation time and evaluated the degree of
photodegradation of polymer substrates.
Results
and Discussion
Characterization of the
TiO2 Layer
Deposited on Polymer Substrates
Figure shows the SEM images of TiO2 coatings
deposited on silicon, PMMA, and PC via AP-PECVD. As we optimized the
deposition conditions (Table ) based on our previous studies[24,25] that were
performed using a Si wafer as the substrate, the purpose of SEM observation
is to confirm the structural similarity of the coatings formed on
different substrates. The TiO2 films had a granular morphology, and the grain size increased
as the deposition time increased. The cross-sectional SEM images indicate
that the thickness of the coated TiO2 film fabricated over
a deposition time of 3 min was around 400 nm. A dense layer was formed
at the bottom of the TiO2 films. It is expected that this
dense layer will prevent incoming UV rays from reaching the coated
surface and protect the polymers from damage. SEM observations showed
no obvious differences in the morphology of the TiO2 coatings
on silicon, PMMA, and PC, although it is well known that the morphology
of coatings is influenced by the substrate properties. The possible
reason may be because the morphological difference caused by substrates
was only pronounced at the initial stage but diminished gradually
with an increase in deposition time since the substrate was gradually
covered by TiO2.
Figure 1
SEM images of TiO2-coated silicon,
PMMA, and PC via
AP-PECVD.
Table 1
Deposition Conditions
of TiO2 Coating on Polymer Substrates
plasma working
gas
Ar, 5 L min–1
precursor carrier gas
Ar, 0.5 L min–1
bubbler temperature
25 °C
TTIP
vapor pressure[47]
6.0 Pa
substrate temperature
50 °C
distance
between the nozzle
and the substrate
5 mm
SEM images of TiO2-coated silicon,
PMMA, and PC via
AP-PECVD.The Fourier transform infrared (FTIR) absorbance
spectra of PMMA
and PC before and after coating with TiO2 are shown in Figure . It should be noted
that the thicknesses of PMMA and PC formed on the silicon wafer were
approximately 3 and 1.5 μm, respectively. The FTIR peaks in Figure a at 2951, 1732,
1448, and 1149 cm–1 assigned to the bands of C–H,
C=O, O–CH3, and C–O–C,[26] respectively, were observed for both samples.
A new peak at 400–800 cm–1, which can be
assigned as the Ti–O bond from the amorphous nature of TiO2,[27] was detected for the TiO2-coated samples. This peak was also confirmed for the TiO2 film coated on silicon (Figure S1 in the Supporting Information). Therefore, the result indicates
that TiO2 was indeed coated on PMMA by AP-PECVD. Similarly,
as shown in Figure b, the FTIR peaks at 2969, 1775, 1503, and 1229 cm–1 correspond to C–H, C=O, C=C, and C–O
from PC,[28] respectively. Whereas, a peak
in the region of 400–800 cm–1 corresponds
to Ti–O from TiO2.[27] This
shows that TiO2-coated PC was fabricated. Moreover, for
TiO2 coatings supported by silicon, a broad peak in the
wavenumber range of 400–800 cm–1 can also
be observed. Furthermore, it is worth noting that there was no difference
in the peak intensity of the polymers with and without TiO2 coatings, and this suggests that the polymers were not damaged during
the AP-PECVD process.
Figure 2
FTIR spectra of PMMA (a) and PC (b) before and after TiO2 coating fabricated over a deposition time of 3 min.
FTIR spectra of PMMA (a) and PC (b) before and after TiO2 coating fabricated over a deposition time of 3 min.UV–vis spectra of TiO2-coated
PMMA and PC fabricated
by AP-PECVD are presented in Figure a,b. The spectra of a quartz sheet were subtracted
from the spectra of the samples. The TiO2 coatings fabricated
over a deposition time of 3 min almost completely shielded the UV
light at wavelengths less than 315 nm (UVB and UVC). For PMMA, the
transmittance at 250 nm in the UV light region decreased from 62%
to nearly 0%, and the transmittance at 550 nm in the visible light
region was maintained at a high level of 95%, even after coating with
TiO2. Similar results were observed using PC as the substrate.
The transmittance at 250 nm decreased from 26% to nearly 0%, and the
transmittance at 550 nm was maintained at 95%. These results demonstrate
that TiO2 coatings fabricated via AP-PECVD can significantly
block UVC and UVB light, and the coatings cause only a slight decrease
in the transparency of the polymers.
Figure 3
UV–vis spectra of TiO2-coated PMMA and PC fabricated
using AP-PECVD (a, b) over a deposition time of 3 min, and UV–vis
spectra of TiO2-coated PMMA and PC fabricated by spin-coating
(c, d) with the following fabrication parameters: TiO2 sol
(STS-01), a concentration obtained via 7-fold dilution with ethanol,
spin-coating speed of 1500 rpm, and spin-coating time of 10 s.
UV–vis spectra of TiO2-coated PMMA and PC fabricated
using AP-PECVD (a, b) over a deposition time of 3 min, and UV–vis
spectra of TiO2-coated PMMA and PC fabricated by spin-coating
(c, d) with the following fabrication parameters: TiO2 sol
(STS-01), a concentration obtained via 7-fold dilution with ethanol,
spin-coating speed of 1500 rpm, and spin-coating time of 10 s.The adhesion strength of the TiO2 coatings
to polymers
was evaluated by comparing the difference in the UV–vis spectra
before and after 1 h of ultrasonication in water and then wiping.
The UV–vis spectra of TiO2-coated polymers by AP-PECVD
before and after ultrasonication and wiping overlapped for both the
TiO2-coated PMMA and the TiO2-coated PC, as
shown in Figure a,b.
This indicates that the TiO2 coatings did not peel off
from the polymer substrates. Therefore, the TiO2 coatings
fabricated via AP-PECVD had good adhesion to PMMA and PC, and the
coatings were also resistant to ultrasonication and wiping.In addition, to buttress our conclusion, the adhesion of TiO2 coatings fabricated via sol–gel spin-coating to different
polymers was also measured using the same process. TiO2 coatings were prepared on PMMA and PC via spin-coating using the
following fabrication parameters:[29,30] TiO2 sol (STS-01, Ishihara Sangyo, Japan, ∼7 nm diameter) was
used under a concentration obtained via 7-fold dilution with ethanol
at the spin-coating speed of 1500 rpm and the spin-coating time of
10 s; the prepared coating was then dried in air overnight. The UV–vis
spectra of PMMA and PC coated with TiO2 via spin-coating
are presented in Figure c,d. The transmittance of PMMA in the UV light region decreased dramatically
after it was coated with TiO2, while no significant change
was observed in the transmittance of PC even after coating with TiO2. This observation shows that the sol–gel-derived TiO2 layer was easily coated on PMMA than on PC. The adhesion
of TiO2 to PC is not as strong as that of PMMA due to the
difference in the number of C=O and C–O groups present
in them.[31] This also explains the better
hydrophobic properties of PC than that of PMMA obtained from the water
contact angle test. Moreover, the UV–vis spectrum of the PMMA
coated with TiO2 via spin-coating changed after ultrasonication
in water for 1 h and wiping; the transmittance in the UV light region
increased due to particle detachment of the TiO2 coating
from PMMA as a result of poor adhesion. A comparison of the change
in transmittance at 250 nm after ultrasonication and wiping (Figure ) also shows enhanced
adhesion of the TiO2 coating to the polymer substrate fabricated
by AP-PECVD than the one fabricated by spin-coating.
Figure 4
Change in transmittance
at 250 nm after ultrasonication and wiping
of TiO2-coated PMMA and PC prepared by AP-PECVD and the
spin-coating method.
Change in transmittance
at 250 nm after ultrasonication and wiping
of TiO2-coated PMMA and PC prepared by AP-PECVD and the
spin-coating method.These results indicate
that the TiO2 coatings fabricated
via AP-PECVD show good adhesion regardless of the substrate. We have
also confirmed that the TiO2 coating on PC maintained the
UV-absorbing performance even after folding and flattening, indicating
good adhesion between TiO2 coating and PC (Figure S2 in the Supporting Information). This
is likely due to the plasma exposure of the polymer substrate in the
initial stage of deposition before a uniform coating of TiO2 covered the substrate.[21] This can lead
to the formation of polar groups that can improve the hydrogen and
covalent bonds as well as the van der Waals interactions. It can also
intensify the creation of chain ends that can enhance interdiffusion
and induce a change in the surface topography, which, in turn, could
improve the mechanical interlocking between the coatings and polymers.[32−34]
Light Absorption Property of the AP-PECVD-Derived
TiO2 Layer
The transmittance values at 250 and
550 nm (Trans.250 and Trans.550), which correspond to the UV and visible
light regions, respectively, of TiO2 coating fabricated
over different deposition times on different substrates, including
quartz, PMMA, and PC, are plotted in Figure . In Figure , the transmittance of only the TiO2 coatings
was compared by subtracting the absorption of the corresponding substrates.
Trans.250 of the TiO2 coatings decreased from approximately
8% to nearly 0% when the deposition time increased from 1 to 5 min.
This observation is due to the increase in the film thickness that
followed the Beer–Lambert law, as discussed in our previous
study.[24,25] Trans.550 decreased from approximately 95
to 90% as the deposition time increased. This is because of the increase
in surface roughness.[25] TiO2 coatings with smaller Trans.250 and larger Trans.550 are preferable
because they show a stronger ability to block UV light and higher
transparency in the visible light region. It is worthy to note that
the Trans.250 value of the TiO2 coatings fabricated for
3 min is as small as the coatings prepared for 5 min, and these coatings
also show a Trans.550 value that is as large as that of the coatings
fabricated for 1 min. Therefore, the TiO2 coatings fabricated
over a 3 min deposition time were suitable for improving the polymer
stability against UV irradiation without decreasing the transparency
of the polymers. Moreover, it is worth noting that TiO2 coatings supported by different substrates of quartz, PMMA, and
PC had similar Trans.250 and Trans.550 values. This indicates that the TiO2 films coated
on different substrates had similar optical properties, although it
is well known that the coating properties are influenced by the substrate
properties. As discussed in Section 2.1, it is possible that the difference
in coating properties caused by substrates probably became evident
at the initial stage but gradually diminished as the deposition time
increased since the substrate was gradually covered by TiO2.
Figure 5
Transmittance at 250 and 550 nm of TiO2 films supported
by different substrates of quartz, PMMA, and PC (absorption values
of the substrates were subtracted) over a deposition time of 0–5
min.
Transmittance at 250 and 550 nm of TiO2 films supported
by different substrates of quartz, PMMA, and PC (absorption values
of the substrates were subtracted) over a deposition time of 0–5
min.
Stability
Improvement against UV Irradiation
PMMA and PC with and without
TiO2 coatings were irradiated
at different UV irradiation times in the range of 0–5 h, and
the FTIR spectra of the samples were obtained, as shown in Figure . For PMMA and PC
without TiO2 coatings, there was a dramatic decrease in
the peak intensity with an increase in the UV irradiation time. This
indicates that the degradation of PMMA and PC without TiO2 coatings occurred during UV irradiation. We have also confirmed
by laser microscopy that there was an obvious decrease in the thickness
for PMMA films after UV irradiation, as shown in Figure S3 in the Supporting Information. However, for the
polymers with TiO2 coatings, no significant change in the
FTIR peak intensity of PMMA and PC was observed after UV irradiation.
This suggests that the AP-PECVD-derived TiO2 coatings can
effectively protect PMMA and PC from UV degradation. The strongest
peaks in the FTIR spectra of PMMA and PC are 1732 and 1229 cm–1, respectively. To evaluate the degree of UV protection
offered by the TiO2 coatings, we calculated the ratio of
FTIR absorbance intensity at a UV irradiation time t (A) to that at t =
0 (A0) of TiO2-coated PMMA
and PC at 1732 and 1229 cm–1, respectively. The
calculated results are presented in Figure .
Figure 6
FTIR spectra of PMMA (a), TiO2-coated
PMMA (b), PC (c),
and TiO2-coated PC (d) at different UV irradiation times
ranging from 0 to 5 h at the TiO2 deposition time of 3
min.
Figure 7
Ratio of FTIR absorbance intensity at UV irradiation
time t (A) to that at t = 0 (A0) for TiO2-coated
PMMA at 1732 cm–1 (a) and TiO2-coated
PC at 1229 cm–1 (b) in the TiO2 deposition
time range of 0–3 min.
FTIR spectra of PMMA (a), TiO2-coated
PMMA (b), PC (c),
and TiO2-coated PC (d) at different UV irradiation times
ranging from 0 to 5 h at the TiO2 deposition time of 3
min.Ratio of FTIR absorbance intensity at UV irradiation
time t (A) to that at t = 0 (A0) for TiO2-coated
PMMA at 1732 cm–1 (a) and TiO2-coated
PC at 1229 cm–1 (b) in the TiO2 deposition
time range of 0–3 min.As shown in Figure , A/A0 of
PMMA and PC without TiO2 coatings (TiO2 deposition
time was 0 min) decreased dramatically as the UV irradiation time
increased to 5 h, which indicates that PMMA and PC were degraded rapidly
under UV irradiation. It is interesting to note that the degradation
rate of PC was slower than that of PMMA under the same UV irradiation
process. This observation is in line with other reports, and it is
ascribed to a photo-Fries rearrangement in the degradation of PC.[35−37] After coating the films with TiO2 over a 0.5 min deposition
time, both the A/A0 values of PMMA and PC remained high, indicating that the
degradation by UV irradiation was markedly reduced. When the deposition
time of coating the TiO2 layer was increased to 3 min,
the values of A/A0 after the UV irradiation time of 5 h were improved from 0.18
to 0.90 for PMMA, and from 0.36 to 0.86 for PC, compared to those
for polymers without TiO2 coatings, respectively.Generally, the UV-induced degradation rates of PMMA and PC are
first-order,[38,39] that is, d(A/A0)/dt = −k·(A/A0), therefore, the first-order rate plot for the change
in absorbance at 1732 and 1229 cm–1 in the respective
FTIR spectra of PMMA and PC are shown in Figure , and the degradation rate constants, k, were calculated from these results.[38] The degradation rate constants of PMMA decreased from 0.36
to 0.018 h–1 after it was coated with TiO2 films. Similarly, for PC, the degradation rate constant decreased
from 0.23 to 0.029 h–1, which suggests that the
TiO2 coatings fabricated via AP-PECVD effectively protected
the polymers of PMMA and PC from degradation, and it significantly
improved the stability of these polymers against UV irradiation.
Figure 8
First-order
rate plot for the change in the absorbance at 1732
cm–1 in the FTIR spectra of PMMA and TiO2-coated PMMA with a deposition time of 3 min (a), and absorbance
at 1229 cm–1 of PC and TiO2-coated PC
with a deposition time of 3 min (b) under a UV irradiation time ranging
from 0 to 5 h.
First-order
rate plot for the change in the absorbance at 1732
cm–1 in the FTIR spectra of PMMA and TiO2-coated PMMA with a deposition time of 3 min (a), and absorbance
at 1229 cm–1 of PC and TiO2-coated PC
with a deposition time of 3 min (b) under a UV irradiation time ranging
from 0 to 5 h.
Conclusions
The stabilities of PMMA and PC against UV irradiation were significantly
improved by coating them with TiO2 films via AP-PECVD.
TiO2 films with a granular morphology were coated on the
polymers of PMMA and PC, and the Ti–O peak in the FTIR spectra
indicated the successful coating of TiO2 films on the polymers.
The transmittance in the UV light region of PMMA and PC decreased
dramatically after it was coated with TiO2 films; however,
it remained at a high level in the visible light region. TiO2 films coated on different substrates of quartz, PMMA, and PC had
similar optical properties. Moreover, the overlapped UV–vis
spectra and the nearly unchanged transmittance values at 250 and 550
nm of TiO2-coated PMMA and PC before and after ultrasonication
and wiping indicate that the AP-PECVD-derived TiO2 coatings
exhibited good adhesion to the polymers. Finally, the values of A/A0 for PMMA and
PC after the UV irradiation time of 5 h were improved from 0.18 to
0.90, and from 0.36 to 0.86, respectively, after they were coated
with TiO2 for a deposition time of 3 min. The degradation
rate constants of PMMA and PC under UV irradiation decreased from
0.36 to 0.018 h–1 and from 0.23 to 0.029 h–1, respectively, after they were coated with TiO2. This
indicates that the TiO2 coatings fabricated via AP-PECVD
effectively protected the polymers of PMMA and PC from degradation
and significantly improved the stability of these polymers against
UV irradiation.
Experimental Section
Materials
The polymer substrates
used in this study were obtained by spin-coating PMMA and PC onto
a silicon wafer (thickness 280 ± 20 μm, orientation P ⟨100⟩)
and a quartz sheet (thickness 1 mm, fused). The polymersspin-coated
on silicon wafers were used for Fourier transform infrared (FTIR)
and scanning electron microscopy (SEM) measurements, while the polymersspin-coated on quartz sheets were used for UV–vis spectroscopic
analysis. PMMA powder and PC pellets were purchased from Tokyo Chemical
Industry and Acros Organics, respectively. Toluene (99.5%) and chloroform
(99%), which were used as the solvents for spin-coating of PMMA and
PC, respectively, were purchased from Sigma-Aldrich and used without
further purification. The titanium(IV) isopropoxide (TTIP, 97%) precursor
for coating TiO2[40−42] was purchased from Sigma-Aldrich.
Preparation of PMMA and PC Substrates
For
the spin-coating of PMMA, a solution with a concentration of
10 wt % was prepared by dissolving PMMA powder in toluene. The spin-coating
speed was 3000 rpm and spin-coating time was 60 s.[43,44] Similarly, for the spin-coating of PC, a solution with a concentration
of 6 wt % was prepared by dissolving PC pellets in chloroform. The
spin-coating speed was 2500 rpm and spin-coating time was 20 s.[45,46] The spin-coated PMMA and PC were cured at room temperature overnight
and the samples were further placed in an oven for 2 h at 80 and 60
°C, respectively.
AP-PECVD Coating of TiO2 on Polymers
The TiO2 coating was conducted
using an AP-PECVD system
using an atmospheric-pressure plasma jet generator (damage-free multi-gas
plasma jet, Plasma Factory Corporation, Japan). The details of the
film preparation procedure are described in one of our previous studies.[25] The deposition conditions used in this study
are presented in Table . The substrate temperature was set to 50 °C to avoid thermal
degradation of the polymer substrate. To eliminate the effect of plasma
stability in the initial stage, rotatable shielding was used to stop
the deposition of TiO2 film during the first 1 min of the
AP-PECVD process.
Characterization of TiO2-Coated
Polymers
Scanning electron microscopy (SEM, Hitachi S-4800)
was used to determine the morphologies of the TiO2-coated
polymers. Fourier transform infrared (FTIR, Jasco FT/IR-4100) spectroscopy
was used to confirm the chemical structure of the polymers and TiO2-coated polymers. UV–vis transmission spectra were
measured using a UV–vis–NIR spectrophotometer (Shimadzu
UV-3600 plus). The level of adhesion of TiO2 on the surface
of the polymers was evaluated by comparing the difference in the UV–vis
spectra before and after ultrasonication in water using an ultrasonic
cleaner (100 kHz, AS ONE VS-100 III),[48−50] and wiping using a paper
for experimental use (S-200, Nippon Paper Crecia Corporation). The
stabilities of polymers with and without TiO2 coatings
against UV irradiation were measured using the changes in the FTIR
absorbances of the polymers under UV irradiation from a UV lamp. The
UV lamp was purchased from Sun Energy Corporation (DGM2501A-01, Japan).
The samples were placed below the UV lamp at a distance of 5 cm, and
the average spectral irradiance density was 1.6 mW cm–2 nm–1 in the UV light region ranging from 200 to
400 nm.
Authors: Uwe R Kortshagen; R Mohan Sankaran; Rui N Pereira; Steven L Girshick; Jeslin J Wu; Eray S Aydil Journal: Chem Rev Date: 2016-08-23 Impact factor: 60.622
Authors: Linying Cui; Alpana N Ranade; Marvi A Matos; Liam S Pingree; Theo J Frot; Geraud Dubois; Reinhold H Dauskardt Journal: ACS Appl Mater Interfaces Date: 2012-12-10 Impact factor: 9.229