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Synthesis of large surface area LaFeO3 nanoparticles by SBA-16 ...

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J Nanopart Res<br />

a<br />

La3d<br />

50<br />

Intensity (a.u.)<br />

800°C<br />

3d 5/2<br />

3d 3/2<br />

DRS (%)<br />

40<br />

30<br />

20<br />

10<br />

900°C<br />

800°C<br />

700°C<br />

600°C<br />

b<br />

Intensity (a.u.)<br />

Intensity (a.u.)<br />

820 830 840 850 860<br />

Binding energy (eV)<br />

c<br />

700°C<br />

800°C<br />

700°C<br />

2p 3/2<br />

2p 1/2<br />

700 710 720 730<br />

Binding energy (eV)<br />

800°C<br />

700°C<br />

524 528 532 536<br />

Binding energy (eV)<br />

Fe2p<br />

wavelength range from 300 to 550 nm, with a SPS peak<br />

at about 390 nm, which can be attributed to the<br />

photoinduced electronic transitions from the valence<br />

band to conduction band (O 2p ? Fe 3d ) (Li et al. 2000).<br />

O L<br />

O L<br />

O H<br />

O H<br />

O1s<br />

Fig. 6 XPS spectra <strong>of</strong> La3d (a), Fe2p (b), and O1s (c) <strong>of</strong><br />

LaFeO 3 samples calcined at 700 and 800 °C<br />

0<br />

300 350 400 450 500 550 600 650 700<br />

Wavelength (nm)<br />

Fig. 7 UV–Vis DRS spectra <strong>of</strong> LaFeO 3 samples calcined at<br />

different temperature<br />

Moreover, the SPS response becomes much stronger<br />

with increasing calcination temperature, which is close<br />

related to the increase in the crystallinity <strong>of</strong> the LaFeO 3 .<br />

The high crystallinity makes electronic band perfect so<br />

as to enhance the built-in field strength, which can<br />

promote charge separation, meanwhile leading to the<br />

decrease <strong>of</strong> the defect amounts, which is also favorable<br />

for charge separation (Jing et al. 2006). According to the<br />

SPS method principles, it can be expected that the<br />

stronger is the SPS signal, the higher is the photoinduced<br />

charge separation rate. Thus, it can be supposed<br />

that the high crystallinity is favorable for the photoinduced<br />

charge separation and then improve the photocatalytic<br />

activity further.<br />

Photocatalytic activity evaluation<br />

The activity <strong>of</strong> the as-prepared LaFeO 3 was evaluated<br />

<strong>by</strong> photocatalytic degradation <strong>of</strong> Rhodamine B solution<br />

under visible light. Figure 9 shows the RhB<br />

degradation rate <strong>of</strong> photocatalytic reaction under<br />

visible irradiation and adsorption in the dark on the<br />

different LaFeO 3 samples and internationally commercial<br />

P-25 TiO 2 . As the calcination temperature is<br />

enhanced, it can be noticed that the photocatalytic<br />

activity <strong>of</strong> the as-prepared LaFeO 3 gradually increases,<br />

and the LaFeO 3 calcined at 900 °C exhibits excellent<br />

photocatalytic activity. Interestingly, all the LaFeO 3<br />

samples display higher visible activity than P25 TiO 2<br />

and those LaFeO 3 samples prepared via the citrate<br />

method (Li et al. 2007). Based on the above discussion,<br />

the high photocatalytic activity is mainly explained<br />

from the following two aspects. One is the <strong>large</strong> <strong>surface</strong><br />

123

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