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Low-Temperature Mineralisation of Titania-Siloxane Composite Layers

Abstract

This paper deals with low-temperature mineralisation of coatings made with titania-siloxane compositions (TSC). Methyltriethoxysilane has been adopted as the precursor for the siloxane, and during its synthesis, an oligomeric siloxane condensate with methyl moieties acting as TiO2 binder has been produced. These methyl moieties, contained in TSC, provide solubility and prevent gelling, but reduce the hydrophilicity of the system, reduce the transfer of electrons and holes generated in the TiO2. In order to avoid these unfavourable effects, TSC mineralisation can be achieved by nonthermal treatment, for example, by using UV-radiation or plasma treatment. Characterisation of the siloxane was performed by gel permeation chromatography (GPC), which showed the size of the siloxane chain. Thermogravimetric analysis revealed a temperature at which the siloxane mineralises to SiO2. Printed layers of two types of TSC with different siloxane contents were studied by a scanning electron microscope (SEM), where a difference in the porosity of the samples was observed. TSC on fluorine-doped tin oxide (FTO) coated glass and microscopic glass were treated with non-thermal UV and plasma methods. TSC on FTO glass were tested by voltammetric measurements, which showed that the non-thermally treated layers have better properties and the amount of siloxane in the TSC has a great influence on their efficiency. Samples on microscopic glass were subjected to a photocatalytic decomposition test of the model pollutant Acid orange 7 (AO7). Non-thermally treated samples show higher photocatalytic activity than the raw sample.

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Low-Temperature Mineralisation of Titania-Siloxane Composite Layers

Author: Svoboda, Tomáš; Veselý, Michal; Bartoš, Radim; Homola, Tomáš; Dzik, Petr
Publisher: MDPI
Year: 2021
DOI: 10.3390/catal11010050
Source: https://dspace.vut.cz/bitstreams/6a89214f-6639-46c2-b5d9-c05f9ba75665/download
ca alys s
A icle
Low-Tempe a u e Mine alisa ion o Ti ania-Siloxane
Composi e Laye s
Tomáš S oboda 1,*, Michal Veselý1, Radim Ba oš 1, Tomáš Homola 2and Pe Dzik 1


Ci a ion: S oboda, T.; Veselý, M.;
Ba oš, R.; Homola, T.; Dzik, P.
Low-Tempe a u e Mine alisa ion o
Ti ania-Siloxane Composi e Laye s.
Ca alys s 2021,11, 50. h ps://
doi.o g/10.3390/ca al11010050
Recei ed: 12 Oc obe 2020
Accep ed: 4 Decembe 2020
Published: 1 Janua y 2021
Publishe ’s No e: MDPI s ays neu-
al wi h ega d o ju isdic ional clai-
ms in published maps and ins i u io-
nal a ilia ions.
Copy igh : © 2021 by he au ho s. Li-
censee MDPI, Basel, Swi ze land.
This a icle is an open access a icle
dis ibu ed unde he e ms and con-
di ions o he C ea i e Commons A -
ibu ion (CC BY) license (h ps://
c ea i ecommons.o g/licenses/by/
4.0/).
1Facul y o Chemis y, B no Uni e si y o Technology, Pu kyˇno a 118, 612 00 B no, Czech Republic;
[email p o ec ed] (M.V.); [email p o ec ed].cz (R.B.); [email p o ec ed] (P.D.)
2Depa men o Physical Elec onics, Facul y o Science, Masa yk Uni e si y, Ko lᡠská267/2, 611 37 B no,
Czech Republic; [email p o ec ed]
*Co espondence: [email p o ec ed]
Abs ac :
This pape deals wi h low- empe a u e mine alisa ion o coa ings made wi h i ania-
siloxane composi ions (TSC). Me hyl ie hoxysilane has been adop ed as he p ecu so o he
siloxane, and du ing i s syn hesis, an oligome ic siloxane condensa e wi h me hyl moie ies ac ing
as TiO
2
binde has been p oduced. These me hyl moie ies, con ained in TSC, p o ide solubili y
and p e en gelling, bu educe he hyd ophilici y o he sys em, educe he ans e o elec ons
and holes gene a ed in he TiO
2
. In o de o a oid hese un a ou able e ec s, TSC mine alisa ion
can be achie ed by non he mal ea men , o example, by using UV- adia ion o plasma ea men .
Cha ac e isa ion o he siloxane was pe o med by gel pe mea ion ch oma og aphy (GPC), which
showed he size o he siloxane chain. The mog a ime ic analysis e ealed a empe a u e a
which he siloxane mine alises o SiO
2
. P in ed laye s o wo ypes o TSC wi h di e en siloxane
con en s we e s udied by a scanning elec on mic oscope (SEM), whe e a di e ence in he po osi y
o he samples was obse ed. TSC on luo ine-doped in oxide (FTO) coa ed glass and mic oscopic
glass we e ea ed wi h non- he mal UV and plasma me hods. TSC on FTO glass we e es ed
by ol amme ic measu emen s, which showed ha he non- he mally ea ed laye s ha e be e
p ope ies and he amoun o siloxane in he TSC has a g ea in luence on hei e iciency. Samples
on mic oscopic glass we e subjec ed o a pho oca aly ic decomposi ion es o he model pollu an
Acid o ange 7 (AO7). Non- he mally ea ed samples show highe pho oca aly ic ac i i y han he
aw sample.
Keywo ds: i anium oxide; me hyl ie hoxysilane; siloxane; plasma ea men ; UV ea men ; AO7
1. In oduc ion
The pho oca aly ic laye s a e nowadays o g ea in e es o wa e [
1
] and ai [
2
]
pu i ica ion. Ti anium dioxide (TiO
2
) laye s a e pa icula ly popula because o hei
ela i ely high e iciency, non- oxici y, and a o dabili y. TiO
2
ha e been widely applied o
con aminan emedia ion and mic oo ganism des uc ion [3,4].
TiO
2
is o en used as a coa ing on ha d and du able ma e ials such as glass. Recen ly,
he e has been an in e es in deposi ing i on lexible subs a es such as polyu e hanes,
polyes e s, poly inyl chlo ides, and o he s, o pho o ol aic, ex ile, and pape indus ies,
and o he s. The main p oblem is he s abilisa ion o TiO
2
on he subs a e in o de no o
elease i om he pho oca aly ic laye in o he en i onmen [
4
–
6
]. Gene ally, he mal me h-
ods o hund eds o deg ees Celsius [
7
] a e used o inc ease he adhesion and pho oca aly ic
ac i i y. Ano he p oblem lies in he TiO2pho oca aly ic ac i i y ha dis u bs he o ganic
ma e ials on o which TiO2is deposi ed. The main di ec ions o he esea ch a e o p o ec
he subs a es om UV and pho oca aly ic deg ada ion, o ensu e su icien pene a ion
o he pollu an s o he pho oca alys , o p o ide lexibili y, and o de elop he p ocess o
p epa ing such a pho oca aly ic sys em ha could be used on an indus ial scale [6,8].
Ca alys s 2021,11, 50. h ps://doi.o g/10.3390/ca al11010050 h ps://www.mdpi.com/jou nal/ca alys s
Ca alys s 2021,11, 50 2 o 13
One way o p o ec he subs a e om deg ada ion by he mal ea men s and pho o-
ca aly ic p ocesses is o use a sui able binde as a ma ix. The ma ix se es as a mechanical
suppo o TiO
2
and as a p o ec i e laye o he subs a e. Howe e , he bonding o he
binde i sel may no be a su icien condi ion o a unc ional pho oca aly ic laye . O he
ea men s a e needed ha may also be he mal ea men s, bu i would be possible o use
he pho oca aly ic p ocesses hemsel es in he laye using UV-i adia ion o sho - e m
exposu e o plasma o low- empe a u e ea men .
Many a eas ex ensi ely use mesopo ous oxide hin ilms as unc ional and s uc-
u al ma e ials. They include p o ec i e and low-dielec ic cons an laye s, selec i e gas
pe mea ion memb anes, we abili y laye s, and gas senso s [9–11].
In his wo k we de eloped and in es iga ed polysiloxane as he TiO
2
ancho ma ix
and we ob ain he i ania-siloxane composi ion (TSC), which can be used o deposi ion on
lexible subs a es wi hou he need o he mal ea men s which damage he subs a e.
Siloxane (oligome o polyme ) can be ob ained om o ganosilicon p ecu so s, which
can be u he doped wi hTiO
2
pa icles. Siloxane se es as a ma ix o ancho ing TiO
2
,
and, a he same ime, i can e ain po osi y o success ully adso b he pollu an s o he
su ace o he pho oca alys g ains deposi ed deepe in he laye [
6
,
12
]. The siloxane used
in his s udy con ains a ce ain p opo ion o me hyl moie ies ha p o ide solubili y and
p e en gelling. On he o he hand, he me hyl moie ies educe he ans e o elec ons
gene a ed by he TiO
2
and signi ican ly de e io a es he pho oca aly ic ac i i y o TiO
2
.
The e is also a ce ain p opo ion o hyd oxyl g oups in siloxanes. The hyd oxyl g oup, as a
esidual g oup, induces mois u e adso p ion h ough hyd ogen bonding when exposed o
mois u e [
13
]. Mois u e (H
2
O) is an impo an pa o he pho oca aly ic p ocesses aking
place in i anium dioxide. Mois e u e-binding hyd oxyl g oups imp o e he we abili y
o he su ace and he pho oca aly ic ac i i y i sel and is a be e supply o pollu an s in
he aqueous medium [
14
]. In o de o emo e he o ganic ma e om he siloxane and
imp o e he ans e o he elec ons, siloxane mus be comple ely mine alised owa ds
amo phous silica su ace. This s ep is adi ionally pe o med by he mal annealing a
hund eds o
◦
C. On he o he hand, his app oach is no compa ible i lexible and he mally-
sensi i e subs a es such as polye hylene e eph hala e (PET) and polye hylene naph hala e
(PEN) a e used. Low-cos subs a es a e a o able o u u e gene a ion manu ac u e o
eme ging echnologies, including lexible and p in ed elec onics. The e o e, i is impo an
o in es iga e no el low- empe a u e me hods compa ible wi h apid and low- empe a u e
pos - ea men o siloxanes as eplacemen s o adi ional he mal annealing ha is no
compa ible wi h lexible elec onics.
In his wo k we also in es iga ed wo non- he mal me hods o pos -p ocessing
o i ania-siloxane composi ion (TSC) laye s: UV-i adia ion and open-ai plasma. UV-
i adia ion was al eady success ully es ed o he ab ica ion o amo phous TiO
2
hin ilms.
UV-i adia ion a oom empe a u e leads o a highe conduc ion band minimum le el
o he ilm and a smalle amoun o hyd oxyl g oup a he ilm su ace, compa ed o he
he mal-assis ed (100–250
◦
C) UV-annealing o he he mal-only annealing (500
◦
C). [
15
].
Plasma ea men can be used o calcina ion and emo al o o ganic esidues om sol–gel
and gene a ion o mesopo ous ilms [
16
–
20
]. The plasma echnique is mo e a ac i e
because i has many ad an ages, such as low p ocessing empe a u e, sho p ocessing
ime and inexpensi e equipmen [9].
We s udied he p ope ies o TSC in syne gy wi h UV-i adia ion and plasma ea men
as he echniques o non- he mal cu ing o pho oca aly ic laye s o imp o e pho oca aly ic
ac i i y. The main pa ame e o he mine alisa ion o siloxane was he s udy o he dec ease
o me hyl g oups by he Fou ie - ans o m in a ed spec oscopy (FT-IR) me hod. The
pho oca aly ic ac i i y was moni o ed by ol amme ic measu emen s and pho oca aly ic
deg ada ion o AO7.
Ca alys s 2021,11, 50 3 o 13
2. Resul s and Discussion
2.1. Viscosi y o Siloxane Solu ions
Figu e 1shows iscosi y o siloxane solu ions es ed wi h a ious concen a ion o
me hanol anging om 10% o 50%. All solu ions es ed show linea dependence o dy-
namic iscosi y wi h shea a e. The sample wi h 50% o e hanol showed a sligh de ia ion
om New onian beha iou (a he lowes shea a e he e is a sign o iscosi y inc ease).
The iscosi y o he solu ions inc eases conside ably as he concen a ion inc eases, which
is impo an , especially o he u u e p in ing o composi ions con aining siloxane.
Ca alys s 2021, 11, x FOR PEER REVIEW 3 o 13
2. Resul s and Discussion
2.1. Viscosi y o Siloxane Solu ions
Figu e 1 shows iscosi y o siloxane solu ions es ed wi h a ious concen a ion o
me hanol anging om 10% o 50%. All solu ions es ed show linea dependence o dy-
namic iscosi y wi h shea a e. The sample wi h 50% o e hanol showed a sligh de ia ion
om New onian beha iou (a he lowes shea a e he e is a sign o iscosi y inc ease).
The iscosi y o he solu ions inc eases conside ably as he concen a ion inc eases, which
is impo an , especially o he u u e p in ing o composi ions con aining siloxane.
0200 400 600 800 1000
0.005
0.010
0.015
0.020
0.025
10 %
20 %
30 %
40 %
50 %
Dynamic iscosi y (Pas)
Shea a e (s–1)
Figu e 1. Viscosi y o siloxane solu ions in absolu e e hanol (concen a ions 10, 20, 30, 40, 50%).
2.2. Su ace Tension o Siloxane Solu ions
We also in es iga ed he e ec o applying concen a ions o e hanol on he su ace
ension o siloxane solu ions. The pu e e hanol has a su ace ension o 21.90 mN·m−1 a 25
°C [21]. The esul s in Table 1 show ha he e was no signi ican change in he su ace
ension o solu ions wi h a ious concen a ion o e hanol. Howe e , wi h he dec easing
concen a ion o pu e e hanol, a sligh inc ease in su ace ension occu s when he concen-
a ion o siloxane in olume, and hence on he su ace o he liquid, inc eases. We see a
ce ain simila i y wi h e hanol, conside ing he possible s uc u e o siloxane (Equa ions
(1) and (2)) whe e R−Si−(OH)3 is p esen in he solu ion, and because in ou case R means
me hyl, he hyd oca bon esidue will no ha e he weigh o signi ican ly a ec he su ace
ension. I can he e o e be assumed ha he su ace ension o he esul ing siloxane-
blended composi ions will no be signi ican ly a ec ed by he amoun o siloxane.
Table 1. Su ace ension o siloxane solu ions (concen a ions 10, 20, 30, 40, 50%).
Concen a ion (%)
10
20
30
40
50
Su ace ension (mN∙m−1)
22.58
22.96
23.52
24.08
24.75
2.3. Gel Pe mea ion Ch oma og aphy
Gel pe mea ion ch oma og aphy (GPC) esul s a e shown in Table 2. The polydis-
pe si y is close o 1, which means ha he pa icles in solu ion ha e simila dimensions,
exp essed by he adius o gy a ion and he weigh a e age mola mass.
Figu e 1. Viscosi y o siloxane solu ions in absolu e e hanol (concen a ions 10, 20, 30, 40, 50%).
2.2. Su ace Tension o Siloxane Solu ions
We also in es iga ed he e ec o applying concen a ions o e hanol on he su ace
ension o siloxane solu ions. The pu e e hanol has a su ace ension o 21.90 mN
·
m
−1
a 25
◦
C [
21
]. The esul s in Table 1show ha he e was no signi ican change in he
su ace ension o solu ions wi h a ious concen a ion o e hanol. Howe e , wi h he
dec easing concen a ion o pu e e hanol, a sligh inc ease in su ace ension occu s when
he concen a ion o siloxane in olume, and hence on he su ace o he liquid, inc eases.
We see a ce ain simila i y wi h e hanol, conside ing he possible s uc u e o siloxane
(Equa ions (1) and (2)) whe e R
−
Si
−
(OH)
3
is p esen in he solu ion, and because in ou
case R means me hyl, he hyd oca bon esidue will no ha e he weigh o signi ican ly
a ec he su ace ension. I can he e o e be assumed ha he su ace ension o he
esul ing siloxane-blended composi ions will no be signi ican ly a ec ed by he amoun
o siloxane.
Table 1. Su ace ension o siloxane solu ions (concen a ions 10, 20, 30, 40, 50%).
Concen a ion (%) 10 20 30 40 50
Su ace ension (mN·m−1)22.58 22.96 23.52 24.08 24.75
2.3. Gel Pe mea ion Ch oma og aphy
Gel pe mea ion ch oma og aphy (GPC) esul s a e shown in Table 2. The polydis-
pe si y is close o 1, which means ha he pa icles in solu ion ha e simila dimensions,
exp essed by he adius o gy a ion and he weigh a e age mola mass.
Ca alys s 2021,11, 50 4 o 13
Table 2.
The esul s o GPC. The polydispe si y is close o 1, which means ha he pa icles in
solu ion ha e simila sizes.
Dilu ion o
10% Solu ion
Injec ion Volume
(µL) MW(kDa) Polydispe si y
(MW/MN)
Radius o
Gy a ion (nm)
1:1 100 1.497 1.019 12.8
1:1 100 1.534 1.036 11.9
1:1 100 1.475 1.033 12.0
1:1 100 1.506 1.046 12.5
Diame e MW(kDa) 1.52 1.032 13
Selec i e s anda d
de ia ion 0.04 0.009 2
2.4. Speci ic Su ace A ea (SSA) and SEM o Siloxane/TiO2
Two siloxane/TiO
2
composi ions o a ios 1:1 and 1:3 we e c ea ed and compa ed.
SSA was measu ed by by ni ogen adso p ion using he BET iso he m (Figu e 2). The wo
di e en alues o siloxane/TiO
2
a ios ha e a di ec impac o he laye ex u al p ope ies
as is e iden om Figu e 3. The mo e i ania ich o mula ion exhibi ed a lu y ex u e
wi h many accessible oids while he mo e binde ich o mula ion is appa en ly dense
and mo e compac . SSA o siloxane/TiO
2
composi ions o a ios 1:1 and 1:3 was calcula ed
as 12.3 m
2
/g and 34.9 m
2
/g, espec i ely. The ques ion o phase composi ion o bo h
coa ings was add essed sepa a ely in ou p e ious communica ion [
22
] and we ound ou
ha binde mine alisa ion p ocess has no impac on he c ys allini y o i ania.
Ca alys s 2021, 11, x FOR PEER REVIEW 4 o 13
Table 2. The esul s o GPC. The polydispe si y is close o 1, which means ha he pa icles in so-
lu ion ha e simila sizes.
Dilu ion o
10% Solu ion
Injec ion Volume
(μL)
MW (kDa)
Polydispe si y
(MW/MN)
Radius o Gy-
a ion (nm)
1:1
100
1.497
1.019
12.8
1:1
100
1.534
1.036
11.9
1:1
100
1.475
1.033
12.0
1:1
100
1.506
1.046
12.5
Diame e MW (kDa)
1.52
1.032
13
Selec i e s anda d de-
ia ion
0.04
0.009
2
2.4. Speci ic Su ace A ea (SSA) and SEM o Siloxane/TiO2
Two siloxane/TiO2 composi ions o a ios 1:1 and 1:3 we e c ea ed and compa ed.
SSA was measu ed by by ni ogen adso p ion using he BET iso he m (Figu e 2). The wo
di e en alues o siloxane/TiO2 a ios ha e a di ec impac o he laye ex u al p ope ies
as is e iden om Figu e 3. The mo e i ania ich o mula ion exhibi ed a lu y ex u e
wi h many accessible oids while he mo e binde ich o mula ion is appa en ly dense
and mo e compac . SSA o siloxane/TiO2 composi ions o a ios 1:1 and 1:3 was calcula ed
as 12.3 m2/g and 34.9 m2/g, espec i ely. The ques ion o phase composi ion o bo h coa -
ings was add essed sepa a ely in ou p e ious communica ion [22] and we ound ou ha
binde mine alisa ion p ocess has no impac on he c ys allini y o i ania.
0.0 0.1 0.2 0.3
0
20
40
60
80
100
1:1
1:3
1/[W((P0/P)–1)] (g–1)
Rela i e p essu e, P/P0
Figu e 2. Mul i-poin BET plo o siloxane/TiO2 wi h a ious a io 1:1 and 1:3.
Figu e 2. Mul i-poin BET plo o siloxane/TiO2wi h a ious a io 1:1 and 1:3.
Ca alys s 2021, 11, x FOR PEER REVIEW 5 o 13
Figu e 3. SEM images. (A) Shows a less po ous laye wi h a siloxane/TiO2 a io o 1:1, and (B) shows a much mo e po ous
laye o a 1:3 a io.
2.5. The mal T ea men o TSC and TGA, DTG
The coa ings we e u he sin e ed in u nace o en a empe a u e 450 °C o 30 min
o mine alise he binde , i.e., emo e he o ganic me hyl moie ies and suppo he
anspo o elec ons om TiO2. FT-IR esul s showed in Figu e 4 e ealed ha siloxane
was no mine alised comple ely. Peaks loca ed a 2995−2950 cm−1 and 2895−2840 cm−1 co -
esponding o asymme ical and symme ical s e ching o −CH3 and indica ing he p es-
ence o me hyl g oups in polysiloxane binde .
3600 3400 3200 3000 2800
0.00
0.01
0.02
0.03
0.04
0.05
Abso bance
Wa enumbe (cm–1)
Un ea ed
450 °C
–CH3
Figu e 4. FT-IR measu emen o TSC on soda-lime glass. The p ocessing empe a u e o 450 °C
was no su icien o mine alise he siloxane because he me hyl g oups a e s ill p esen a e he -
mal ea men .
The coa ings we e u he analysed by DSC-TGA and hea ed o 1300 °C. Du ing he
he mal p ocess, he e we e se e al changes as he empe a u e ose (Figu e 5). The i s
ange was om 20 °C o 477 °C. The e was p obably a loss o so bed ai mois u e o e-
sidual sol en . Weigh dec eases s eeply. The second majo change occu s a 478 °C, when
he e was a u he apid d op in weigh . Siloxane should be calcined a his empe a u e
and hus deg ade he p ima ily me hyl g oups bonded o silicon oxide. Ano he weigh
change was signi ican ly slowed down om a empe a u e o 600 °C un il i s abilised and
no changes occu ed. I is clea om he measu emen s ha , o comple e calcina ion, i is
necessa y o achie e empe a u es highe han 478 °C, and he e o e, he he mal me hod
o mine alisa ion is only sui able o esis an ma e ials.
Figu e 3.
SEM images. (
A
) Shows a less po ous laye wi h a siloxane/TiO
2
a io o 1:1, and (
B
) shows a much mo e po ous
laye o a 1:3 a io.
Ca alys s 2021,11, 50 5 o 13
2.5. The mal T ea men o TSC and TGA, DTG
The coa ings we e u he sin e ed in u nace o en a empe a u e 450
◦
C o 30 min
o mine alise he binde , i.e., emo e he o ganic me hyl moie ies and suppo he anspo
o elec ons om TiO
2
. FT-IR esul s showed in Figu e 4 e ealed ha siloxane was
no mine alised comple ely. Peaks loca ed a 2995
−
2950 cm
−1
and 2895
−
2840 cm
−1
co esponding o asymme ical and symme ical s e ching o
−
CH
3
and indica ing he
p esence o me hyl g oups in polysiloxane binde .
Ca alys s 2021, 11, x FOR PEER REVIEW 5 o 13
Figu e 3. SEM images. (A) Shows a less po ous laye wi h a siloxane/TiO2 a io o 1:1, and (B) shows a much mo e po ous
laye o a 1:3 a io.
2.5. The mal T ea men o TSC and TGA, DTG
The coa ings we e u he sin e ed in u nace o en a empe a u e 450 °C o 30 min
o mine alise he binde , i.e., emo e he o ganic me hyl moie ies and suppo he
anspo o elec ons om TiO2. FT-IR esul s showed in Figu e 4 e ealed ha siloxane
was no mine alised comple ely. Peaks loca ed a 2995−2950 cm−1 and 2895−2840 cm−1 co -
esponding o asymme ical and symme ical s e ching o −CH3 and indica ing he p es-
ence o me hyl g oups in polysiloxane binde .
3600 3400 3200 3000 2800
0.00
0.01
0.02
0.03
0.04
0.05
Abso bance
Wa enumbe (cm–1)
Un ea ed
450 °C
–CH3
Figu e 4. FT-IR measu emen o TSC on soda-lime glass. The p ocessing empe a u e o 450 °C
was no su icien o mine alise he siloxane because he me hyl g oups a e s ill p esen a e he -
mal ea men .
The coa ings we e u he analysed by DSC-TGA and hea ed o 1300 °C. Du ing he
he mal p ocess, he e we e se e al changes as he empe a u e ose (Figu e 5). The i s
ange was om 20 °C o 477 °C. The e was p obably a loss o so bed ai mois u e o e-
sidual sol en . Weigh dec eases s eeply. The second majo change occu s a 478 °C, when
he e was a u he apid d op in weigh . Siloxane should be calcined a his empe a u e
and hus deg ade he p ima ily me hyl g oups bonded o silicon oxide. Ano he weigh
change was signi ican ly slowed down om a empe a u e o 600 °C un il i s abilised and
no changes occu ed. I is clea om he measu emen s ha , o comple e calcina ion, i is
necessa y o achie e empe a u es highe han 478 °C, and he e o e, he he mal me hod
o mine alisa ion is only sui able o esis an ma e ials.
Figu e 4.
FT-IR measu emen o TSC on soda-lime glass. The p ocessing empe a u e o 450
◦
C was no
su icien o mine alise he siloxane because he me hyl g oups a e s ill p esen a e he mal ea men .
The coa ings we e u he analysed by DSC-TGA and hea ed o 1300
◦
C. Du ing he
he mal p ocess, he e we e se e al changes as he empe a u e ose (Figu e 5). The i s
ange was om 20
◦
C o 477
◦
C. The e was p obably a loss o so bed ai mois u e o esidual
sol en . Weigh dec eases s eeply. The second majo change occu s a 478
◦
C, when he e
was a u he apid d op in weigh . Siloxane should be calcined a his empe a u e and
hus deg ade he p ima ily me hyl g oups bonded o silicon oxide. Ano he weigh change
was signi ican ly slowed down om a empe a u e o 600
◦
C un il i s abilised and no
changes occu ed. I is clea om he measu emen s ha , o comple e calcina ion, i is
necessa y o achie e empe a u es highe han 478 ◦C, and he e o e, he he mal me hod
o mine alisa ion is only sui able o esis an ma e ials.
Ca alys s 2021, 11, x FOR PEER REVIEW 6 o 13
Figu e 5. The esul s o he TGA, DTG. The mine alisa ion and emo al o he me hyl g oups om
he siloxane should occu a 478 °C.
2.6. FT-IR o Non he mal Cu ing TSC
UV-i adia ion and non- he mal a mosphe ic-p essu e plasma ea men we e u -
he in es iga ed in o de o eplace ime-consuming he mal sin e ing, which is p oblem-
a ic i polysiloxane/TiO2 is deposi ed on he mally-sensi i e ma e ials. Bo h siloxane/TiO2
composi ions o a ios 1:1 and 1:3 we e in es iga ed by FT-IR be o e and a e UV-i adi-
a ion and plasma ea men .
Figu e 6A,B shows FT-IR spec a o siloxane/TiO2 laye s p epa ed by bo h composi-
ions o a ios 1:1 and 1:3, cu ed by UV-i adia ion o 0–210 min. The dec ease o peaks
ela ed o asymme ical and symme ical s e ching o −CH3 (2995−2950 cm−1 and
2895−2840 cm−1) indica e he emo al o −CH3 g oups om siloxane su ace and appa -
en ly he ans o ma ion o siloxane owa ds amo phous SiO2. Fo bo h coa ings (1:1 and
1:3 a io), UV-i adia ion o 150 min was enough o emo e all de ec able −CH3 g oups.
This dec ease can be u he explained by pho oca aly ical eac ion be ween ana ase TiO2
wi h bandgap 3.2 eV [23] ha can p o ide addi ional ca aly ical eac ion on polysiloxane
su ace and enhance he deg ada ion o me hyl g oups.
Figu e 6C,D shows FT-IR spec a o siloxane/TiO2 laye s p epa ed by bo h composi-
ions o a ios 1:1 and 1:3, cu ed by plasma o 0–32 s. In con as wi h he esul s p esen ed
o UV-i adia ed laye s, he plasma ea ed laye s showed signi ican ly lowe e iciency
o me hyl g oups emo al. The mos p o ound di e ence was ound o he ilm o lowe
po osi y (1:1) and highe e iciency was ound o he laye o highe po osi y. This dis-
c epancy is clea ly ela ed o he di e ence in mechanism o UV-i adia ion and plasma
ea men . Whe eas he dominan ene gy- ans e mechanism in UV-i adia ion is he
anspo o pho ons o ce ain wa eleng h in o he po ous ilm, he plasma ea men
wo ks di e en ly. Apa om he UV-i adia ion, he plasma gene a ed a a mosphe ic
p essu e in ambien ai con ains a ious ene ge ic species ha can ca y ene gy owa ds
siloxane su ace: High- empe a u e elec ons, low- empe a u e ions, exci ed species and
me as ables. These species, howe e , ecombine and ex inc in con ac wi h ma e ials su -
ace and hus, he po osi y o ma e ial plays an impo an ole in he limi a ion o such
me hod. Since plasma ea men was less e icien o me hyl emo al a less po ous ma-
e ial, i can be concluded ha plasma canno e icien ly pene a e in o he coa ing bulk
and mine alise i . On he o he hand, he coa ing wi h high po osi y showed be e e i-
ciency o me hyl emo al, and he e o e, i is impo an o ind an op imal combina ion o
laye po osi y i a mosphe ic p essu e plasma is used o mine alisa ion o coa ings. Al -
hough no e icien as UV-i adia ion, a clea bene i o plasma ea men is in signi ican ly
as e ea men imes, in o de o en seconds, which allow o use his me hod on as oll-
o- oll p oduc ion lines and employ he coa ings in lexible and p in ed elec onics con-
cep .
Figu e 5.
The esul s o he TGA, DTG. The mine alisa ion and emo al o he me hyl g oups om
he siloxane should occu a 478 ◦C.

Ca alys s 2021,11, 50 6 o 13
2.6. FT-IR o Non he mal Cu ing TSC
UV-i adia ion and non- he mal a mosphe ic-p essu e plasma ea men we e u he
in es iga ed in o de o eplace ime-consuming he mal sin e ing, which is p oblema ic
i polysiloxane/TiO
2
is deposi ed on he mally-sensi i e ma e ials. Bo h siloxane/TiO
2
composi ions o a ios 1:1 and 1:3 we e in es iga ed by FT-IR be o e and a e UV-i adia ion
and plasma ea men .
Figu e 6A,B shows FT-IR spec a o siloxane/TiO
2
laye s p epa ed by bo h com-
posi ions o a ios 1:1 and 1:3, cu ed by UV-i adia ion o 0–210 min. The dec ease o
peaks ela ed o asymme ical and symme ical s e ching o
−
CH
3
(2995
−
2950 cm
−1
and
2895
−
2840 cm
−1
) indica e he emo al o
−
CH
3
g oups om siloxane su ace and appa -
en ly he ans o ma ion o siloxane owa ds amo phous SiO
2
. Fo bo h coa ings (1:1 and
1:3 a io), UV-i adia ion o 150 min was enough o emo e all de ec able
−
CH
3
g oups.
This dec ease can be u he explained by pho oca aly ical eac ion be ween ana ase TiO
2
wi h bandgap 3.2 eV [
23
] ha can p o ide addi ional ca aly ical eac ion on polysiloxane
su ace and enhance he deg ada ion o me hyl g oups.
Ca alys s 2021, 11, x FOR PEER REVIEW 7 o 13
3600 3400 3200 3000 2800
0.02
0.04
0.06
FT-IR (UV 0–210 min)
siloxane/TiO2 (1:1)
0 min
15 min
30 min
60 min
90 min
150 min
210 min
Abso bance
Wa enumbe (cm–1)
–CH3
3600 3400 3200 3000 2800
0.00
0.02
0.04
0.06
FT-IR (UV 0–210 min)
siloxane/TiO2 (1:3)
0 min
15 min
30 min
60 min
90 min
150 min
210 min
Abso bance
Wa enumbe (cm–1)
–CH3
(A)
(B)
3600 3400 3200 3000 2800
0.02
0.04
0.06 0 s
2 s
4 s
8 s
16 s
32 s
Abso bance
Wa enumbe (cm–1)
FT-IR (plasma 0–32 s)
siloxane/TiO2 (1:1)
–CH3
3600 3400 3200 3000 2800
0.01
0.02
0.03
0.04
0.05
0.06
0.07
0.08
FT-IR (plasma 0–32 s)
siloxane/TiO2 (1:3)
0 s
2 s
4 s
8 s
16 s
32s
Abso bance
Wa enumbe (cm–1)
–CH3
(C)
(D)
Figu e 6. FT-IR measu emen s o TSC laye s. (A,B) a e images o samples ea ed wi h UV-i adia ion; (C,D) a e images
o plasma- ea ed samples. UV-i adia ion has be e laye pene a ion and is he e o e e ec i e o laye s wi h a highe
concen a ion o siloxane.
2.7. Vol amme ic Measu emen s o Non he mal Cu ing TSC
Vol amme ic measu emen s can be aken o he pho oca aly ic ac i i y es . I he
ea ed laye is exposed o UV-i adia ion, i gene a es an elec on/hole pai . By applying
he ex e nal ol age, he elec ons can be abs ac ed om he exci on and he pho ocu en
is de ec ed in he ex e nal ci cui . The g ow h o he pho ocu en is ela ed o highe pho-
oca aly ic ac i i y [24].
The siloxane/TiO2 ilms o a ios 1:1 and 1:3 we e exposed o UV-i adia ion o 0–
120 min and plasma ea men o 0–32 s. Figu e 7 shows he ol ame ic measu emen o
pho ocu en gene a ed by he coa ing upon exposu e o UV. The UV-i adia ion p e-
ea men o 0–120 min led o a g adual inc ease o he pho ocu en o bo h coa ings
(1:1, 1:3) in es iga ed. Highe alues o pho ocu en we e measu ed o coa ing wi h a
highe concen a ion o TiO2 in siloxane/TiO2 ( a io 1:3). This is appa en ly hanks o
highe concen a ion o pho o-ca aly ically ac i e TiO2 ha can no only imp o e he min-
e alisa ion eac ion, bu also supply mo e elec ons upon UV exposu e. Fu he mo e, he
po osi y o he coa ing wi h siloxane/TiO2 a io 1:3 is highe , so he highe pho ocu en is
mos likely an in e play be ween hese ac o s.
Figu e 7C,D shows ol amme ic measu emen s o siloxane/TiO2 ilms o a ios 1:1
and 1:3 we e exposed o ai plasma o 0–32 s. The coa ing wi h small po osi y yields e y
Figu e 6.
FT-IR measu emen s o TSC laye s. (
A
,
B
) a e images o samples ea ed wi h UV-i adia ion; (
C
,
D
) a e images
o plasma- ea ed samples. UV-i adia ion has be e laye pene a ion and is he e o e e ec i e o laye s wi h a highe
concen a ion o siloxane.
Figu e 6C,D shows FT-IR spec a o siloxane/TiO
2
laye s p epa ed by bo h composi-
ions o a ios 1:1 and 1:3, cu ed by plasma o 0–32 s. In con as wi h he esul s p esen ed
o UV-i adia ed laye s, he plasma ea ed laye s showed signi ican ly lowe e iciency
Ca alys s 2021,11, 50 7 o 13
o me hyl g oups emo al. The mos p o ound di e ence was ound o he ilm o lowe
po osi y (1:1) and highe e iciency was ound o he laye o highe po osi y. This dis-
c epancy is clea ly ela ed o he di e ence in mechanism o UV-i adia ion and plasma
ea men . Whe eas he dominan ene gy- ans e mechanism in UV-i adia ion is he
anspo o pho ons o ce ain wa eleng h in o he po ous ilm, he plasma ea men
wo ks di e en ly. Apa om he UV-i adia ion, he plasma gene a ed a a mosphe ic
p essu e in ambien ai con ains a ious ene ge ic species ha can ca y ene gy owa ds
siloxane su ace: High- empe a u e elec ons, low- empe a u e ions, exci ed species and
me as ables. These species, howe e , ecombine and ex inc in con ac wi h ma e ials
su ace and hus, he po osi y o ma e ial plays an impo an ole in he limi a ion o such
me hod. Since plasma ea men was less e icien o me hyl emo al a less po ous ma e-
ial, i can be concluded ha plasma canno e icien ly pene a e in o he coa ing bulk and
mine alise i . On he o he hand, he coa ing wi h high po osi y showed be e e iciency
o me hyl emo al, and he e o e, i is impo an o ind an op imal combina ion o laye
po osi y i a mosphe ic p essu e plasma is used o mine alisa ion o coa ings. Al hough
no e icien as UV-i adia ion, a clea bene i o plasma ea men is in signi ican ly as e
ea men imes, in o de o en seconds, which allow o use his me hod on as oll- o- oll
p oduc ion lines and employ he coa ings in lexible and p in ed elec onics concep .
2.7. Vol amme ic Measu emen s o Non he mal Cu ing TSC
Vol amme ic measu emen s can be aken o he pho oca aly ic ac i i y es . I he
ea ed laye is exposed o UV-i adia ion, i gene a es an elec on/hole pai . By applying
he ex e nal ol age, he elec ons can be abs ac ed om he exci on and he pho ocu en
is de ec ed in he ex e nal ci cui . The g ow h o he pho ocu en is ela ed o highe
pho oca aly ic ac i i y [24].
The siloxane/TiO
2
ilms o a ios 1:1 and 1:3 we e exposed o UV-i adia ion o
0–120 min
and plasma ea men o 0–32 s. Figu e 7shows he ol ame ic measu emen
o pho ocu en gene a ed by he coa ing upon exposu e o UV. The UV-i adia ion p e-
ea men o 0–120 min led o a g adual inc ease o he pho ocu en o bo h coa ings
(1:1, 1:3) in es iga ed. Highe alues o pho ocu en we e measu ed o coa ing wi h
a highe concen a ion o TiO
2
in siloxane/TiO
2
( a io 1:3). This is appa en ly hanks
o highe concen a ion o pho o-ca aly ically ac i e TiO
2
ha can no only imp o e he
mine alisa ion eac ion, bu also supply mo e elec ons upon UV exposu e. Fu he mo e,
he po osi y o he coa ing wi h siloxane/TiO
2
a io 1:3 is highe , so he highe pho ocu en
is mos likely an in e play be ween hese ac o s.
Figu e 7C,D shows ol amme ic measu emen s o siloxane/TiO
2
ilms o a ios 1:1
and 1:3 we e exposed o ai plasma o 0–32 s. The coa ing wi h small po osi y yields
e y small pho ocu en s, and i seems ha plasma ea men had a nega i e e ec on he
maximal pho ocu en alues. On he o he hand, he plasma ea men o he coa ing wi h
highe po osi y (1:3) esul ed in a g adual inc ease in pho ocu en wi h plasma-exposu e
ime. The be e e iciency in pho ocu en gene a ion in he coa ing o highe po osi y is
ela ed o highe mine alisa ion e iciency, as shown in FT-IR esul s p esen ed in
Figu e 6D.
Ca alys s 2021,11, 50 8 o 13
Ca alys s 2021, 11, x FOR PEER REVIEW 8 o 13
small pho ocu en s, and i seems ha plasma ea men had a nega i e e ec on he max-
imal pho ocu en alues. On he o he hand, he plasma ea men o he coa ing wi h
highe po osi y (1:3) esul ed in a g adual inc ease in pho ocu en wi h plasma-exposu e
ime. The be e e iciency in pho ocu en gene a ion in he coa ing o highe po osi y is
ela ed o highe mine alisa ion e iciency, as shown in FT-IR esul s p esen ed in Figu e
6D.
-0.5 0.0 0.5 1.0 1.5 2.0
0
10
20
30
40
50
0 min
15 min
30 min
60 min
90 min
120 min
Pho ocu en (mA)
Po en ial s. FTO (V)
UV 0–120 min, siloxane/TiO2 (1:1)
-0.5 0.0 0.5 1.0 1.5 2.0
0
10
20
30
40
50
60
70
80
Pho ocu en (mA)
0 min
15 min
30 min
60 min
90 min
120 min
Po en ial s. FTO (V)
UV 0–120 min, siloxane/TiO2 (1:3)
(A)
(B)
-0.5 0.0 0.5 1.0 1.5 2.0
0
10
20
30
40
50
0 s
2 s
4 s
8 s
16 s
32 s
Pho ocu en (mA)
Po en ial s. FTO (V)
Plasma 0–32 s, siloxane/TiO2 (1:1)
0.0 0.5 1.0 1.5 2.0
0
5
10
15
20
25
30
35
40
45
50
0 s
2 s
4 s
8 s
16 s
32 s
Pho ocu en (mA)
Po en ial s. FTO (V)
Plasma 0–32 s, siloxane/TiO2 (1:3)
(C)
(D)
Figu e 7. Vol amme ic cha ac e isa ion o TSC p in ed on FTO-coa ed glass. (A,B) a e images o samples ea ed wi h
UV-i adia ion; (C,D) a e images o plasma- ea ed samples. Plasma can no pene a e he laye su icien ly i i con ains
oo much siloxane. In he case o (C), he pho ocu en is e y low o ze o.
2.8. Pho oca aly ic Deg ada ion o Acid O ange 7
Acid O ange 7 (AO7) se es as a model pollu an o he pho odeg ada ion es . AO7
u ns he aqueous solu ion o o ange and i is a esis an subs ance ha slow deg ades.
Figu e 8 shows he dec ease in abso bance signal e lec ing he concen a ion o AO7 upon
i adia ion o UVA o 1 h. UVA was chosen because adia ion wi h lowe wa eleng hs is
less ad an ageous in e ms o ene gy e iciency. We compa ed h ee samples wi h a io
1:3: un ea ed siloxane/TiO2, UV-i adia ed siloxane/TiO2 o 210 min and plasma- ea ed
siloxane/TiO2 o 32 s. The slowes deg ada ion o AO7 was obse ed o un ea ed silox-
ane/TiO2, whe eas he as es deg ada ion was obse ed o UV-i adia ed siloxane/TiO2
o 210 min. The plasma- ea ed siloxane/TiO2 showed signi ican imp o emen in AO7
Figu e 7.
Vol amme ic cha ac e isa ion o TSC p in ed on FTO-coa ed glass. (
A
,
B
) a e images o samples ea ed wi h
UV-i adia ion; (
C
,
D
) a e images o plasma- ea ed samples. Plasma can no pene a e he laye su icien ly i i con ains
oo much siloxane. In he case o (C), he pho ocu en is e y low o ze o.
2.8. Pho oca aly ic Deg ada ion o Acid O ange 7
Acid O ange 7 (AO7) se es as a model pollu an o he pho odeg ada ion es . AO7
u ns he aqueous solu ion o o ange and i is a esis an subs ance ha slow deg ades.
Figu e 8shows he dec ease in abso bance signal e lec ing he concen a ion o AO7
upon i adia ion o UVA o 1 h. UVA was chosen because adia ion wi h lowe wa e-
leng hs is less ad an ageous in e ms o ene gy e iciency. We compa ed h ee samples
wi h a io 1:3: un ea ed siloxane/TiO
2
, UV-i adia ed siloxane/TiO
2
o 210 min and
plasma- ea ed siloxane/TiO
2
o 32 s. The slowes deg ada ion o AO7 was obse ed o
un ea ed siloxane/TiO
2
, whe eas he as es deg ada ion was obse ed o UV-i adia ed
siloxane/TiO
2
o 210 min. The plasma- ea ed siloxane/TiO
2
showed signi ican imp o e-
men in AO7 deg ada ion in compa ison o he un ea ed sample, al hough he e iciency
o siloxane/TiO
2
i adia ed by UV was be e . I should be no ed ha UVA in ol ed in
AO7 deg ada ion es may u he con ibu e o mine alisa ion o TSC [25].
Ca alys s 2021,11, 50 9 o 13
Ca alys s 2021, 11, x FOR PEER REVIEW 9 o 13
deg ada ion in compa ison o he un ea ed sample, al hough he e iciency o silox-
ane/TiO2 i adia ed by UV was be e . I should be no ed ha UVA in ol ed in AO7 deg-
ada ion es may u he con ibu e o mine alisa ion o TSC [25].
0500 1000 1500 2000 2500 3000 3500
0.35
0.40
0.45
0.50
Blank
Raw
Plasma 32 s
UV 210 min
Abso bance
Time (s)
Figu e 8. Deg ada ion o 2 mg/L aqueous solu ion o AO7 wi h immobilized TSC laye s ea ed by
plasma and UV-i adia ion.
3. Ma e ials and Me hods
3.1. Syn hesis o Siloxane
The s a ing subs ance o he syn hesis o siloxane was me hyl ie hoxysilane
(MTEOS) (Al a Aesa , 98%, Ha e hill, MA, USA). MTEOS was hyd olysed wi h acidic
wa e . E hanol was o med du ing he hyd olysis and subsequen ly dis illed. Siloxane
was ex ac ed wi h die hyl e he (Pen a, 99.7%), and i was dissol ed in absolu e e hanol
(Pen a, 99.8%, P ague, Czech Republic) a e e apo a ion o he ex ac ing agen . The si-
loxane solu ion in e hanol was s o ed a a empe a u e below 0 °C [6]. The expec ed chem-
ical eac ion can be summa ised by he ollowing equa ion [26]:
   
OHH3COHSiRO3HHOCSiR52
3
2
3
52 
(1)
     
OHROHSiOOHSiROHSi2R 2
223 -----
(2)
3.2. P epa a ion o TSC
Two se ies o samples we e p epa ed o expe imen s, as shown in Table 3. TiO2 (P25,
Sigma Ald ich, 99.7%, S . Louis, MO, USA, pa icle size ≤ 25 nm, SSA 45–55 m2/g [27]) was
dispe sed in dowanol and a siloxane 20% solu ion was added. The esul ing suspension
was u he dilu ed wi h hexanol. The TSC we e p in ed wi h a Dima ix (DMP-2800) ma-
e ial p in e on soda-lime glass and FTO-coa ed glass.
Table 3. Composi ions designed o ma e ial p in ing.
Composi ion
Siloxane (20% in E hanol)
TiO2 (20% P25 in Dowanol)
Hexanol
E38-9AD (1:1)
4 mL
4 mL
20 mL
E38-10AD (1:3)
2 mL
6 mL
20 mL
3.3. Mine alisa ion o he P in ed TSC on he Subs a e
The siloxane/TiO2 coa ings we e mine alised by wo me hods: UV-i adia ion and
plasma ea men . UV-i adia ion was gene a ed by a Syl ania UV lamp Figu e 9 (me -
cu y, 125 W, Budapes , Hunga y). The adia ion in ensi y was se and held a 9 mW∙cm−2.
Figu e 8.
Deg ada ion o 2 mg/L aqueous solu ion o AO7 wi h immobilized TSC laye s ea ed by
plasma and UV-i adia ion.
3. Ma e ials and Me hods
3.1. Syn hesis o Siloxane
The s a ing subs ance o he syn hesis o siloxane was me hyl ie hoxysilane (MTEOS)
(Al a Aesa , 98%, Ha e hill, MA, USA). MTEOS was hyd olysed wi h acidic wa e . E hanol
was o med du ing he hyd olysis and subsequen ly dis illed. Siloxane was ex ac ed
wi h die hyl e he (Pen a, 99.7%), and i was dissol ed in absolu e e hanol (Pen a, 99.8%,
P ague, Czech Republic) a e e apo a ion o he ex ac ing agen . The siloxane solu ion in
e hanol was s o ed a a empe a u e below 0
◦
C [
6
]. The expec ed chemical eac ion can be
summa ised by he ollowing equa ion [26]:
R−Si(OC2H5)3+3H2O→R−Si(OH)3+3C2H5OH (1)
2R −Si(OH)3↔R−Si(OH)2−O−Si(OH)2−R+H2O (2)
3.2. P epa a ion o TSC
Two se ies o samples we e p epa ed o expe imen s, as shown in Table 3. TiO
2
(P25,
Sigma Ald ich, 99.7%, S . Louis, MO, USA, pa icle size
≤
25 nm, SSA 45–55 m
2
/g [
27
]) was
dispe sed in dowanol and a siloxane 20% solu ion was added. The esul ing suspension
was u he dilu ed wi h hexanol. The TSC we e p in ed wi h a Dima ix (DMP-2800)
ma e ial p in e on soda-lime glass and FTO-coa ed glass.
Table 3. Composi ions designed o ma e ial p in ing.
Composi ion Siloxane (20% in E hanol) TiO2(20% P25 in Dowanol) Hexanol
E38-9AD (1:1) 4 mL 4 mL 20 mL
E38-10AD (1:3) 2 mL 6 mL 20 mL
3.3. Mine alisa ion o he P in ed TSC on he Subs a e
The siloxane/TiO
2
coa ings we e mine alised by wo me hods: UV-i adia ion and
plasma ea men . UV-i adia ion was gene a ed by a Syl ania UV lamp Figu e 9(me cu y,
125 W, Budapes , Hunga y). The adia ion in ensi y was se and held a 9 mW
·
cm
−2
.
Samples we e placed unde 5 mm o dis illed wa e and i adia ed o 0, 15, 30, 60, 90, 150,
and 210 min.