Xufei Shao1,2, Xiaotong Li2,3, Jinzhu Ma2,4,3, Runduo Zhang1, Hong He2,4,3. 1. State Key Laboratory of Chemical Resource Engineering, Beijing Key Laboratory of Energy Environmental Catalysis, Beijing University of Chemical Technology, Beijing 100029, China. 2. State Key Joint Laboratory of Environment Simulation and Pollution Control, Research Center for Eco-Environmental Sciences, Chinese Academy of Sciences, Beijing 100085, China. 3. University of Chinese Academy of Sciences, Beijing 100049, China. 4. Center for Excellence in Regional Atmospheric Environment, Institute of Urban Environment, Chinese Academy of Sciences, Xiamen 361021, China.
Abstract
Ozone is a poisonous gas, so it is necessary to remove excessive ozone in the environment. Catalytic decomposition is an effective way to remove ozone at room temperature. In this work, 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 catalysts were synthesized by the impregnation method. The 10%Ag/nano-Al2O3 catalyst showed 89% ozone conversion for 40 ppm O3 for 6 h under a space velocity of 840 000 h-1 and a relative humidity of 65%, which is superior to 10%Ag/AlOOH-900 (45% conversion). The characterization results showed Ag nanoparticles to be the active sites for ozone decomposition, which were more highly dispersed on nano-Al2O3 as a result of the greater density of terminal hydroxyl groups. The understanding of the dispersion and valence of silver species gained in this study will be beneficial to the design of more efficient supported silver catalysts for ozone decomposition in the future.
Ozone is a poisonous gas, so it is necessary to remove excessive ozone in the environment. Catalytic decomposition is an effective way to remove ozone at room temperature. In this work, 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 catalysts were synthesized by the impregnation method. The 10%Ag/nano-Al2O3 catalyst showed 89% ozone conversion for 40 ppm O3 for 6 h under a space velocity of 840 000 h-1 and a relative humidity of 65%, which is superior to 10%Ag/AlOOH-900 (45% conversion). The characterization results showed Ag nanoparticles to be the active sites for ozone decomposition, which were more highly dispersed on nano-Al2O3 as a result of the greater density of terminal hydroxyl groups. The understanding of the dispersion and valence of silver species gained in this study will be beneficial to the design of more efficient supported silver catalysts for ozone decomposition in the future.
Due to the deterioration
of the environment, ozone has increasingly
drawn our attention. Outdoors, the photochemical reaction of VOCs
and NO in the atmosphere produces ozone,
which leads to excessive ozone concentrations in the near-surface
troposphere.[1,2] Indoors, air cleaners, printers,
and copiers can release ozone.[3] In 2005,
the World Health Organization (WHO) stipulated that the 8 h average
ozone concentration in the working environment shall not exceed 100
μg/m3. Excessive ozone seriously threatens people’s
health[4] and reduces crop yields.[5] Thus, the disposal of excess ozone is a pressing
problem.There are a variety of methods to remove ozone, such
as active
carbon absorption, liquid absorption, thermal decomposition, and catalytic
decomposition. Among these, catalytic decomposition is considered
to be the most efficient, safe, and economical method. Catalysts for
ozone decomposition mainly include transition metal oxides (e.g.,
MnO,[6−9] CoO,[10] Fe2O3,[11] NiO,[12] and ZnO[13]) and noble metals (e.g., Au,[14,15] Ag,[16−18] Pt,[19] Pd,[20,21] and Rh[22]). However, most transition metal oxides have
the disadvantages of poor moisture resistance and eventual deactivation.
Noble metals can effectively improve the water resistance and increase
the lifetime of the catalysts. Ag-based catalysts are much cheaper
than other noble metal catalysts and are widely used. Ag/perlite,
Ag/SiO2, Ag/α-Al2O3, and Ag/clinoptilolite
have been investigated. The results indicate that Ag species are the
active sites for ozone decomposition.[23−26] Li et al.[16] confirmed that metallic silver particles (Ag0) on Ag–Mn catalysts showed much
better ozone removal performance than Ag1.8Mn8O16 and Agδ+ species. Kumar et al.[27,28] prepared Ag/MCM-41-20,
Ag/H-MCM-41-50, and Ag/H-beta-11 and confirmed that the acidic properties
and structure of catalyst supports had an effect on the state of Ag
on these ozone decomposition catalysts. However, it was not clear
how the support could influence the state of silver and then have
an impact on the activity of catalysts.γ-Al2O3 has often been used as a nonreactive
catalyst support because it is easy to determine the active sites
and the reaction mechanism in catalytic studies. Ag has typically
been used as the active component in catalysts because of its low
price and good performance. Thus, Ag/γ-Al2O3 has been widely studied in a variety of catalytic reactions due
to its excellent performance and easy preparation. Examples include
the catalytic oxidation of HCHO[29,30] and selective catalytic
reduction and selective catalytic oxidation of NO.[31−34] Wang et al.[35] compared the state of Ag
on 1%Ag/nano-Al2O3 and 1%Ag/micro-Al2O3 and found that the use of nano-Al2O3 as a support can lead to single-atom silver dispersion, while
Ag on micro-Al2O3 existed in the form of Ag
clusters. They confirmed that Ag was anchored by terminal hydroxyl
groups and that abundant terminal hydroxyl groups on a support would
result in high dispersion and utilization of Ag.In this work,
we successfully synthesized 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 catalysts by the impregnation method.
The characterization results showed that silver in the metallic state
was a superior active site for ozone decomposition and that the abundant
terminal hydroxyl groups on nano-Al2O3 led to
high dispersion of Ag.
Results and Discussion
Ozone Decomposition Performance
The
ozone decomposition performance of AlOOH-900, nano-Al2O3, 10%Ag/AlOOH-900, and 10%Ag/nano-Al2O3 is displayed in Figure . The AlOOH-900 and nano-Al2O3 supports
had no ozone removal ability at room temperature under the conditions
of 40 ppm ozone concentration and RH = 65%. The results were consistent
with the study of Tao et al.,[21] who found
that the ozone conversion of Al2O3/Al-fiber
was nearly zero. When silver at 10 wt % was supported on AlOOH-900
and nano-Al2O3, the ozone conversion was improved
dramatically. After 6 h, the activity of 10%Ag/nano-Al2O3 was up to 90% and remained stable. However, 10%Ag/AlOOH-900
only exhibited 45% ozone conversion, which was about half that of
10%Ag/nano-Al2O3. The above phenomenon was possibly
related to the state, dispersity, or size of silver species on the
support.
Figure 1
Ozone conversion of nano-Al2O3, AlOOH-900,
10%Ag/nano-Al2O3, and 10%Ag/AlOOH-900; Conditions:
ozone inlet concentration, 40 ppm; temperature, 30 °C; relative
humidity, 65%; and space velocity, 840 000 h–1.
Ozone conversion of nano-Al2O3, AlOOH-900,
10%Ag/nano-Al2O3, and 10%Ag/AlOOH-900; Conditions:
ozone inlet concentration, 40 ppm; temperature, 30 °C; relative
humidity, 65%; and space velocity, 840 000 h–1.
Specific
Surface Area and the Crystal Structure
Figure shows the
N2 adsorption–desorption isotherms, X-ray diffraction
(XRD) patterns, and morphology of the samples. As shown in Figure a, the isotherms
of all samples were type IV with a hysteresis loop of type H3 (according
to IUPAC). There was no change in the type of pore structure after
silver was impregnated on the samples. As shown in Table , the specific surface areas
of nano-Al2O3 and AlOOH-900 were similar, 176.7
and 199.8 m2/g, respectively. The specific surface area
declined after the addition of Ag for both supports, but the area
for 10%Ag/AlOOH-900 was still much larger, indicating that the specific
surface area was not the main factor in the ozone decomposition activity.
As shown in Figure b, nano-Al2O3 and AlOOH-900 had the same crystalline
structure as γ-Al2O3. Figure c,d shows that nano-Al2O3 had a sheet-like morphology with a particle
size of about 10 nm, and AlOOH-900 had a morphology consisting of
sheets and rods longer than 20 nm.
Figure 2
(a) N2 adsorption–desorption
isotherms and pore-size
distribution curves (inset) of nano-Al2O3, AlOOH-900,
10%Ag/nano-Al2O3, and 10%Ag/AlOOH-900; (b) XRD
patterns of nano-Al2O3 and AlOOH-900; (c) high-resolution
transmission electron microscopy (HRTEM) of nano-Al2O3; and (d) HRTEM of AlOOH-900.
Table 1
Brunauer–Emmett–Teller
(BET) Surface Area, Pore Size, and Pore Volume of the Four Samples
sample
SBET [m2/g]
pore diameter (d)
[nm]
pore volume (V) [cm3/g]
nano-Al2O3
176.7
13.5
0.7
AlOOH-900
199.8
13.5
0.8
10%Ag/nano-Al2O3
160.5
13.1
0.6
10%Ag/AlOOH-900
177.0
12.5
0.6
(a) N2 adsorption–desorption
isotherms and pore-size
distribution curves (inset) of nano-Al2O3, AlOOH-900,
10%Ag/nano-Al2O3, and 10%Ag/AlOOH-900; (b) XRD
patterns of nano-Al2O3 and AlOOH-900; (c) high-resolution
transmission electron microscopy (HRTEM) of nano-Al2O3; and (d) HRTEM of AlOOH-900.
Chemical States and Dispersion
of Silver
Figure shows the
XRD patterns of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
The diffraction peaks at 38.1, 44.3, 64.4, and 77.5° correspond
to the (111), (200), (220), and (311) lattice planes of the Ag metal
(JCPDS 87-0717),[34] respectively. Also,
it could be observed that the peak intensity of Ag on 10%Ag/AlOOH-900
was stronger than that on 10%Ag/nano-Al2O3.
The results may be due to the coalescence of some Ag nanoparticles
or a better degree of crystallinity of Ag on AlOOH-900. In addition,
the diffraction peaks at 19.3, 32.3, 33.8, and 37° assigned to
AgO species appeared on 10%Ag/AlOOH-900,
indicating that part of Ag was oxidized and may form AgO particles. Perhaps this was the reason why the ozone
conversion of 10%Ag/AlOOH-900 was worse than that of 10%Ag/nano-Al2O3.
Figure 3
XRD patterns of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
XRD patterns of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.Figure shows the
HRTEM images of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
As shown in Figure a,c, many silver nanoparticles with a size of 4–5 nm were
anchored on nano-Al2O3, displaying an unclear
lattice fringe, but the silver nanoparticles began to coalesce to
form larger particles with a size of 10–15 nm with clearer
lattice fringes on 10%Ag/AlOOH-900, which may have adverse effects
on ozone decomposition. The results further confirmed the above XRD
results. The lattice spacings of Ag nanoparticles on 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 were measured and are shown
in Figure b,d. Fringe
spacings of 0.236 and 0.228 nm on sliver particles may represent the
(111) plane of Ag0 and the
(2̅02) plane of AgO, respectively.[36]
Figure 4
(a,
b) HRTEM image of 10%Ag/nano-Al2O3 and
(c, d) HRTEM image of 10%Ag/AlOOH-900.
(a,
b) HRTEM image of 10%Ag/nano-Al2O3 and
(c, d) HRTEM image of 10%Ag/AlOOH-900.X-ray photoelectron spectroscopy (XPS) spectra were then measured
to confirm the state of silver. Figure a shows the Ag 3d spectra of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900, which showed that the binding
energies of Ag 3d5/2 for 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 were 368.3 and 368.2 eV. The peak of
Ag 3d on 10%Ag/nano-Al2O3 was located at a higher
binding energy, indicating that there was more Ag0 in the Ag nanoparticles. According to the inductively
coupled plasma optical emission spectroscopy (ICP-OES) data in Table , the content of Ag
for 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 in
the bulk was 8.6 and 8.4%, respectively. The Ag content on the surface
of the two catalysts was measured by XPS as 10.97 and 8.94%, respectively,
as shown in Table . The above results indicated that the silver particles were more
dispersed on the surface of nano-Al2O3, which
was consistent with the results of HRTEM and XRD. To determine the
percentage of Ag0 in the silver
particles, the peaks of Ag 3d5/2 were deconvoluted into
two peaks at 368.7 and 367.9 eV, which were deemed as arising from
silver in the metallic and oxidized states[37−39] displayed in Figure b,c. The percentages
of Ag0 in 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 were 53 and 39%, respectively
(Table ), indicating
that 10%Ag/nano-Al2O3 had more Ag in the metallic
state, which was beneficial to ozone removal.[16]
Figure 5
(a)
Ag 3d XPS spectra of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900;
(b) Ag 3d5/2 XPS spectra of 10%Ag/nano-Al2O3; and (c) Ag 3d5/2 XPS spectra of
10%Ag/AlOOH-900.
Table 2
ICP-OES
and XPS Results of Ag Species
of 10%Ag/Nano-Al2O3 and 10%Ag/AlOOH-900
ICP-OES
XPS
sample
Ag (wt %)
Ag (wt %)
Agn0 (%)
Agnδ+ (%)
10%Ag/nano-Al2O3
8.6
10.97
53
47
10%Ag/AlOOH-900
8.4
8.94
39
61
(a)
Ag 3d XPS spectra of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900;
(b) Ag 3d5/2 XPS spectra of 10%Ag/nano-Al2O3; and (c) Ag 3d5/2 XPS spectra of
10%Ag/AlOOH-900.UV–vis DRS spectra
of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 were
obtained by subtracting the spectrum of
bare BaSO4. As can be seen in Figure , all samples have a broad absorption band
from 200 to 700 nm. The bands at 209 and 232 nm can be attributed
to the Ag+ species.[40] The band
at 289 nm is attributed to Agδ+.[41] The broad bands at 364 and 491 nm
belong to Ag0 and AgNPs, respectively.[42] It is obvious that 10%Ag/nano-Al2O3 has a stronger Ag0 absorption band and a weaker AgNPs absorption
band than those of 10%Ag/AlOOH-900. These results indicate that 10%Ag/nano-Al2O3 has more small Ag0 particles in the metallic state, but the Ag species
on 10%Ag/AlOOH-900 coalesce to form larger particles.
Figure 6
UV–vis profiles
of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
UV–vis profiles
of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.H2-Temperature-programmed reduction
(H2-TPR)
(Figure ) was used
to characterize the relative content of Ag in the oxidized state.
The peaks at 117 and 131 °C corresponded to the reduction of
large AgO clusters; the peaks at 199
and 212 °C were due to the reduction of small AgO clusters.[43] Compared
to the 10%Ag/AlOOH-900 catalyst, 10%Ag/nano-Al2O3 had less oxidized Ag and a lower reduction temperature. The AgO species on 10%Ag/nano-Al2O3 were not detected by XRD or HRTEM, possibly due to their
highly dispersed or ultrathin amorphous outer layers over the surface
of silver nanoparticles, and they did not form AgO particles like that on 10%Ag/AlOOH-900.[34,44]
Figure 7
H2-TPR image of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
H2-TPR image of 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900.
Hydroxyl Group Content
The anchoring
mechanism of noble metals on supports has been investigated. The effect
of electronic interactions between reducible oxides and noble metals
was considered to be an important factor affecting metal anchoring
on the supports.[45] However, for nonreducible
supports, there may be other reasons for the anchoring of metal species
on the supports. Kwak et al.[46] reported
that unsaturated pentacoordinate Al3+ (Al3+ penta)
on the surface of γ-Al2O3 was the anchoring
site of Pt. Wang et al.[35] found that terminal
hydroxyl groups on γ-Al2O3 were the anchoring
points of Ag species. To study the anchoring mechanism of Ag on Al2O3 further, in situ diffuse reflectance infrared
spectroscopy (DRIFTS) with NH3 adsorption was performed
to measure the content of OH groups.Figure shows the spectra of in situ DRIFTS with
NH3 adsorption (Figure a) and the peak fitting (Figure b,c) results for the wavenumbers from 3850
to 3590 cm–1. As shown in Figure a, the peak at about 3771 cm–1 was due to terminal hydroxyl groups (type I), the peak at about
3729 cm–1 was derived from doubly bridging hydroxyls
(type II), and the peak at about 3675 cm–1 was due
to triply bridging hydroxyl groups (type III).[35,47,48] Compared with AlOOH-900, nano-Al2O3 had more terminal hydroxyl groups. After Ag was impregnated
on the supports, the peaks for terminal hydroxyls (type I) of nano-Al2O3 and AlOOH-900 decreased sharply and nearly disappeared,
indicating that Ag consumed almost all of the terminal hydroxyl groups
on the supports. The result further indicated that terminal hydroxyl
groups were the main anchoring sites of Ag. Besides, the peak intensity
due to type II hydroxyl groups on 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900 became stronger, which may be because of the
generation of a new type of hydroxyl group after Ag was added to the
surface. There was no change in the peak intensity of type III hydroxyl
groups on nano-Al2O3 and AlOOH-900, indicating
that they were not the main anchoring sites for Ag nanoparticles.
Besides the three kinds of hydroxyl groups (types I, II, and III)
on nano-Al2O3 and AlOOH-900, a peak for a new
type of doubly bridging hydroxyl group generated at about 3748 cm–1, marked as type II′, appeared on 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900, as shown in Figure b,c. To see the proportion
of each hydroxyl group a bit more intuitively, the percentage composition
of each type of hydroxyl group was calculated, as shown in Table . The proportion of
terminal hydroxyl groups (type I) on nano-Al2O3 was 38%, higher than that on AlOOH-900 (15%). As for 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900, type I contents were 10
and 7%, respectively. As indicated by the results above, nano-Al2O3 had more terminal hydroxyl groups available
to anchor Ag particles, which were the active sites of ozone decomposition.
Therefore, the ozone conversion of 10%Ag/nano-Al2O3 was higher than that of 10%Ag/AlOOH-900.
Figure 8
(a) In situ DRIFTS spectra
of NH3 adsorption on the
four samples; (b) peak fitting of OH consumption peaks after in situ
DRIFTS of NH3 adsorption over nano-Al2O3 and 10%Ag/nano-Al2O3; and (c) peak
fitting of OH consumption peaks after in situ DRIFTS of NH3 adsorption over AlOOH-900 and 10%Ag/AlOOH-900.
Table 3
Proportion of OH Consumption for Four
Types of Hydroxyl Groups According to the Peak Fitting Results of
In Situ DRIFTS of NH3 Adsorption
sample
type I (%)
type II (%)
type III (%)
type II′ (%)
nano-Al2O3
38
25
37
AlOOH-900
15
57
28
10%Ag/nano-Al2O3
10
33
39
18
10%Ag/AlOOH-900
7
53
35
5
(a) In situ DRIFTS spectra
of NH3 adsorption on the
four samples; (b) peak fitting of OH consumption peaks after in situ
DRIFTS of NH3 adsorption over nano-Al2O3 and 10%Ag/nano-Al2O3; and (c) peak
fitting of OH consumption peaks after in situ DRIFTS of NH3 adsorption over AlOOH-900 and 10%Ag/AlOOH-900.
Conclusions
This study compared two kinds of Ag-containing catalysts, 10%Ag/nano-Al2O3 and 10%Ag/AlOOH-900, which were prepared by
the impregnation method. The ozone conversion of 10%Ag/nano-Al2O3 was 89%, higher than that of 10%Ag/AlOOH-900
(45%). The characterization results showed that nano-Al2O3 had nearly four times the number of terminal hydroxyl
groups as AlOOH-900, leading to better dispersion of Ag particles
with the metallic state (Ag0), which were superior active sites for ozone decomposition. Thus,
10%Ag/nano-Al2O3 had better ozone removal performance.
The understanding of the dispersion and valence of silver species
detailed in this paper will be beneficial to the design of more efficient
supported silver catalysts for ozone decomposition in the future.
Materials and Methods
Preparation of Catalysts
The AlOOH-900
support was prepared by calcining commercial boehmite at 900 °C
for 3 h, and the nano-Al2O3 support was purchased
(Aladdin). Catalysts with a silver loading of 10% were prepared by impregnating nano-Al2O3 or AlOOH-900 in silver nitrate solution. After stirring
for 2 h on a magnetic stirring apparatus, the sample was evacuated
on a rotary evaporator at 333 K for 1 h until the water evaporated.
Then, the catalysts were dried at 100 °C for about 12 h and calcined
at 500 °C for 3 h in air (Scheme ).
Scheme 1
Catalyst
Characterization
The BET
surface areas and pore properties of the samples were obtained by
a Quantachrome Quadrasorb SI-MP analyzer. The Brunauer–Emmett–Teller
(BET) method was used to calculate the specific surface area of the
samples. The Barrett–Joyner–Halenda (BJH) method was
used to determine the diameter and volume of pores. After outgassing
at 300 °C for 4 h, N2 was adsorbed on the samples
at −196 °C to obtain the adsorption and desorption curves.The crystalline structure of the catalysts was determined by X-ray
powder diffraction (XRD) (D8-Advance, Bruker, Germany) with Cu Kα
radiation (λ = 0.15406 nm) operated at 40 kV and 40 mA. The
scan range was set from 5 to 90° with a step size of 0.02°.High-resolution transmission electron microscopy (HRTEM) images
were obtained on a JEOL JEM 2010 TEM with an acceleration voltage
of 200 kV.The silver content of the catalysts was determined
by an inductively
coupled plasma emission spectrometer (ICP-OES) (720, Varian). The
elemental composition, content, and valence state of species on the
surface of the samples were analyzed by X-ray photoelectron spectra
(XPS) (Axis UItra, Kratos Analytical Ltd., U.K.) using Al Kα
radiation.The valence state of silver was analyzed by diffuse
reflectance
UV–vis spectra. The spectra were measured at room temperature
in air with BaSO4 as reference (U-3100 UV–vis spectrophotometer,
Hitachi Co., Japan) and were collected in the range of 200–700
nm with a resolution of 1 nm.The hydroxyl content was determined
by an in situ DRIFTS system
(Nexus 670, Thermo Nicolet) equipped with an MCT/A detector. Prior
to NH3 absorption (500 ppm), the sample was pretreated
at 350 °C for 1 h in 10%O2/N2 (500 mL/min)
and cooled to room temperature.The relative content of silver
oxide of the catalysts was obtained
by H2 temperature-programmed reduction (H2-TPR)
experiments performed on a Micromeritics Autochem II 2920 equipped
with a thermal conductivity detector (TCD). The samples (100 mg) were
pretreated at 300 °C for 30 min in Ar (30 mL/min) and then were
cooled to 30 °C. Next, after the baseline had stabilized, the
catalysts were heated in 10%H2/Ar (30 mL/min) from 30 to
400 °C (10 °C/min).
Catalysts’
Ozone Decomposition Activity
Catalysts of 40–60 mesh
with a mass of 100 mg were placed
into a fixed-bed continuous flow quartz reactor (i.d., 4 mm). Then,
all of the samples were tested at 30 °C with a gas flow of 1.4
L/min and RH = 65%. The concentration of ozone was 40 ± 2 ppm
and the space velocity was about 840 000 h–1. The ozone was generated by low-pressure ultraviolet lamps, and
the inlet and outlet ozone concentrations were detected by an ozone
monitor (model 202, 2B Technologies). A humidity probe (HMP110, Vaisala
OYJ, Finland) was used to control the humidity at 65%. The formula
used to compute ozone conversion was as followswhere Cin and Cout are the inlet and outlet
concentrations
of ozone, respectively.
Authors: Ja Hun Kwak; Jianzhi Hu; Donghai Mei; Cheol-Woo Yi; Do Heui Kim; Charles H F Peden; Lawrence F Allard; Janos Szanyi Journal: Science Date: 2009-09-25 Impact factor: 47.728
Authors: K Arve; K Svennerberg; F Klingstedt; K Eränen; L R Wallenberg; J-O Bovin; L Capek; D Yu Murzin Journal: J Phys Chem B Date: 2006-01-12 Impact factor: 2.991