G Model
CATTOD-10444; No. of Pages7
ARTICLE IN PRESS
B. Cojocaru et al. / Catalysis Today xxx (2016) xxx–xxx
2
synthesized by the quick hydrolysis of titanium butoxide (reagent
grade, Sigma-Aldrich) by adding drops of DI water into a solution
of titanium butoxide and butanol followed by centrifugation, dry-
◦
ing and calcination at 500 C for 6 h. Then SBA-15, TiO2 NA and
TiO2 were used as the supports for the deposition of Au nanopar-
ticles. To deposit Au nanoparticles, supports were dispersed in
2
00 mL of 6 mM trisodium citrate (premium quality level, Sigma-
Aldrich) aqueous solution and stirred vigorously for 1 h. Then,
0 mL of 3 mMHAuCl4 (99.9% metals basis, Aldrich) aqueous solu-
5
tion was added to the above suspension dropwise and the mixture
was allowed to react overnight under vigorous magnetic stirring.
Finally, the product was centrifuged and cleaned with DI water
◦
Scheme 1. Interfacial charge transfer in Au-TiO2 NPs with Fermi level equilibration.
several times and dried at 100 C for 24 h. Au/meso-TiO2 was syn-
thesized using a one-pot method. In detail, a designated amount
of HAuCl4 was dissolved in 40 mL of butanol and stirred at room
temperature to complete dissolution, then 4 g of poly(ethylene
glycol)-block-poly(propylene glycol)-block-poly(ethylene glycol)
on endocrine disruptors’ toxicology as well as the development of
analytical methods for detection and quantification of EDs con-
taminants at low concentration levels [10–12]. Currently, a new
aspect of the EDs issues is considered such as the environmental
cleanup of ED hazard compounds. A brief search on the literature
shows the scientific interest on EDs remediation, especially cat-
alytic remediation (e.g. photo- remediation) that is continuously
growing.
Among “classical” routes to degrade BPA, the photocatalytic
route is gaining much interest as a green method requiring a
cheap (practically free) energy source and limited only by the
light absorbing capacity of the catalysts. Besides the reference TiO2
(EO20PO70EO20, P123, MW = 5800, Aldrich) was added and stirred
for 30 min. Titanium butoxide solution (20 g of titanium butoxide
in 25 mL of butanol) was added dropwise to the above solution.
◦
Finally, the mixture was aged at 40 C overnight, filtered, dried
◦
and calcined at 500 C for 6 h. The deposition of Au onto Degussa
P25 was carried out following the precipitation-deposition method.
Thus, 1 g of TiO2 Degussa P25 was added to the corresponding vol-
ume of an aqueous solution of HAuCl ·3H O (0.2 M). The pH of the
4
2
solution was stabilized at 8–9 by addition of a 0.2 M NaOH solution.
◦
The mixture was stirred at 80 C for 12 h. After that, the suspension
[
13], “improved” photocatalysts like Ti/TiO2 [14], Pr,N-TiO2 [15],
−
was filtered, washed with water till free of Cl . Finally, the solid
was dried at 80 C for 48 h. Using this procedure samples with 0.1,
H PW12O40/TiO [16], Ag-TiO2 [17], Pt-TiO2 [18] or Photo-Fenton
3
2
◦
systems [19,20] showed a promising behavior for the removal of
BPA.
0
.3, 0.7 and 1 wt% Au, respectively, were obtained.
Gold catalysis has attracted great interest in the past period
[
21]. In addition to the catalytic oxidative reactions, gold nanopar-
2
.2. Catalyst characterization
ticles were found to promote the catalytic activity of TiO2 [22–26].
It has also been observed that the visible light absorbed by gold
nanoparticles due to the surface plasmon resonance is leading to
the generation of photo-excited states of gold nanoparticles fol-
Textural characteristics of the investigated catalysts were deter-
mined from the adsorption-desorption isotherms of nitrogen at
◦
−
196 C using a Micromeritics ASAP 2020 Surface Area and Porosity
[
27]
lowed by the transfer of the electrons to the TiO2
. Thus, the
Analyzer. DR-UV–vis spectra were collected under ambient con-
ditions with a Specord 250 (Analytic Jena) with an integrating
sphere and MgO as reference. The registered spectra were trans-
formed using the Kubelka-Munk F(R) function. The band gap energy
surface plasmon resonance originating from the collective oscil-
lations of the electrons on the surface of the gold nanoparticles
was suggested to be the essential factor of the promoting effect.
The enhanced interfacial charge transfer between TiO2 and gold
resulting from the accumulation of more electrons can be achieved
by a negative shift in the Fermi level of the Au–TiO2 composite
2
was calculated from the dependence of [F(R) • hꢀ] as a func-
tion of hꢀ, were hꢀ is the energy of the incident photons. Raman
spectra were taken with a Horiba Jobin Yvon − Labram HR UV–vis-
NIR (200–1600 nm) Raman Microscope Spectrometer, using a laser
with the wavelength of 632 nm. Powder X-ray Diffraction patterns
were collected at room temperature using a Shimadzu XRD-7000
with Cu K␣ monochromatic radiation ( = 1.5406 Å, 40 kV, 40 mA)
[
22–28]. Metal or metal ion doped semiconductor composites typ-
ically exhibit a shift in the Fermi level to more negative potentials.
This improves the energetics of the composite system and enhances
the efficiency of the interfacial charge-transfer process [22]. For
the particular case of Au/TiO , previous reports already indicated
2
◦
−1
with a scanning rate of 0.1 min , in the 2ꢁ range of 5–80.
XPS spectra were recorded at room temperature using a SSX-100
spectrometer, Model 206 from Surface Science Instrument. The
pressure in the analysis chamber during the analysis was 1.33
mPa. Monochromatized Al-K␣ radiation (hꢀ = 1486.6 eV) generated
by bombarding the Al anode with an electron gun operated with
a beam current of 12 mA and acceleration voltage of 10 kV has
been used. The spectrometer energy scale was calibrated using the
Au 4f7/2 peak centered at 83.98 eV. Charge correction was made
with the C 1 s signal of adventitious carbon (C C or C H bonds)
located at 284.8 eV. The atomic surface compositions were cal-
culated using the sensitivity factors provided with the ESCA 8.3
D software, applied to the surface below the corresponding fit-
ted XPS signals. An estimated error of ± 0.1 eV can be assumed for
all measurements. Specimens for electron microscopy were pre-
recorded on a JEOL JEM ARM 200 F electron microscope operated
the accumulation of more electrons in system [25] having as an
ultimate effect an enhanced photo-catalytic activity (Scheme 1).
The resonances of the surface plasmons are directly affected by the
wavelength, particle size, shape, and local dielectric environment.
Starting from this state of the art, the aim of this study was to
investigate the photo-activity of a series of catalysts containing gold
deposited on titania in the decontamination of water solutions con-
taining BPA and to elucidate the effect of the gold plasmon and of
the nature of the support.
2
. Experimental
2.1. Catalyst preparation
Corporation (NanoActive TiO ) and used as received. TiO2 was
2
Please cite this article in press as: B. Cojocaru, et al., Enhanced photo-degradation of bisphenol pollutants onto gold-modified photo-