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L. Geng et al. / Journal of Catalysis 377 (2019) 145–152
Chemisorption and dissociation are the fundamental steps in
flask. The flask was connected to an air balloon and the mixture
was vigorously stirred at 80 °C for 8 h. Aliquots of the products
were taken with a sampling pipe and analyzed with a gas chro-
matograph equipped with a HP-5 column and FID detector. The
product mixtures were further identified by GC-MS.
A hot filtration test was carried out as follows: After 2 h of reac-
tion, the solid catalysts were separated with a Buchner funnel.
Then the mixture of the filtrate was put into the reactor and con-
tinuously reacted under the same conditions (80 °C, air 1 atm)
without any solid catalyst. In the recycling experiment, the used
catalyst was separated from the reactant by an external magnet
and treated at 350 °C for 1 h in air before the next test cycle.
molecular O2 activation, which are essentially associated with
charge transfer from the active sites of the catalyst to the antibond-
ing molecular orbitals of O2. The crystal phase determines the geo-
metric and electronic structure of a catalyst [41–45], which
significantly affects the bulk and surface charge transport, and ulti-
mately reflects the activity and density of the active sites. In this
work, by investigation of the dependence of catalytic oxidation
on the crystal phases of iron oxides, we find that naked c-Fe2O3
particles (with a magnetically separable character) exhibit excel-
lent catalytic activity, selectivity, and stability for a series of imine
synthesis reactions under mild conditions (even at 40 °C, 1 atm).
Through a combination of experimental characterizations and the-
oretical calculations based on density functional theory (DFT), the
crystal structure effect of iron oxides on O2 activation and catalytic
oxidative coupling behavior is clarified. It is shown that the inverse
2.4. Density functional theory calculation details
All first-principles calculations in this study were performed
within the frame of DFT using the plane-wave pseudopotential
approach and implemented by the Vienna Ab Initio Simulation
Package (VASP). A spin-polarized exchange–correlation functional
was described within the PBE generalized gradient approximation
[47,48], and electron–core interactions were used with projected
augmented wave (PAW) pseudopotentials. The reciprocal space
was spanned with a plane-wave basis cutoff of 400 eV. The Bril-
louin zone was automatically generated by the original Monk
horst–Pack grid, and the k-points for structure optimization were
selected as 3 ꢂ 3 ꢂ 1. In all cases of structural optimization, the
energy convergence was set to 1 ꢂ 10ꢀ4 eV, and the force on the
atoms was less than 0.05 eV/Å.
spinel structure of c-Fe2O3 (with abundant cation vacancies) con-
fers unique electronic properties on surface Fe species. These Fe
species tend to transfer electrons to molecular oxygen to form
Oꢀ2 or O22ꢀ species, which is favorable for high activity of
in the aerobic coupling reaction.
c-Fe2O3
2. Experimental
2.1. Preparation of iron oxide with different crystal phases
Fe3O4 was synthesized via a modified ammonia-assisted precip-
itation method [46]. Typically, Fe chloride precursors (Fe2+/Fe3+
molar ratio = 1:2) were dissolved in an ethanol/water (1:1) solu-
tion under nitrogen with constant mechanical stirring for 30 min,
and a 10% ammonia solution was used to adjust the pH of the solu-
tion to 9.0. The black suspension was then stirred for 1 h at room
temperature and another 1 h at 60 °C in an oil bath. After the sys-
tem was cooled to room temperature, the resulting solids were
separated using a magnet, washed with alcohol, and dried at
Fe3d74s1 and O2s22p4 valence electron configuration were
adopted in this study. To more accurately consider the effect of
the strong correlation of Fe on the 3d electrons, a DFT+U strategy
was used to calculate the electron density. This method also helped
to correct the O2 binding errors [49,50]. In addition, according to
the widely approved values in the literature [51-53], the effective
U-values of Fe and O atoms were set to 4.0 and 0.0 eV, respectively.
Integration over the irreducible part of the Brillouin zone was car-
ried out using the linear tetrahedron method with Bloch correc-
tions, which depict electronic structure more precisely.
Considering the Bader analysis, charges in adsorption are described
as numbers of electrons gained or lost in comparison with the neu-
tral atom [54,55].
80 °C in a vacuum oven.
ment of the synthesized Fe3O4 in air at 350 °C for 2 h.
c
-Fe2O3 was obtained via thermal treat-
-Fe2O3 par-
a
ticles were obtained using a procedure similar to that for Fe3O4
nanoparticles. The difference is that iron chloride hexahydrate
(FeCl3ꢁ6H2O) was used as an Fe precursor and the resulting solids
were finally thermally treated at 550 °C for 2 h in a muffle furnace.
The lattice parameters of a-Fe2O3, Fe3O4, and c-Fe2O3 used in all
calculations are summarized in Table S1 in the Supporting
Information. In view of surface and molecular oxygen activation
2.2. Characterization of catalysts
properties, the {0 0 1}, {1 1 1}, and {1 1 1} facets of
a-Fe2O3, Fe3O4,
Scanning electron microscopy (SEM) images were taken on a
Hitachi-SU8020 with an accelerating voltage of 30 kV. The crystal
and -Fe2O3 were adopted, respectively [56–58]. To eliminate the
c
influence of the thickness of the slab atomic layers, all models were
composed of eight layers of Fe and four layers of O and separated
from periodic images by at least 15 Å of vacuum. Concerning the
significance of the adsorption interface, the top five layers were
relaxed and the following seven layers of atoms were fixed in the
optimization process. The adsorption energy can be expressed as
structures were recorded using
diffractometer (XRD) equipped with a CuK
a
Rigaku powder X-ray
radiation source
a
( k = 1.542 nm). Raman spectra were collected on a Bruker RFS 100
Raman spectrometer with an argon laser (532 nm) as an excitation
source. Fourier transform infrared spectra (FTIR) were recorded on a
Thermo Nicolet 6700 FT-IR spectrometer. 57Fe Mössbauer spectra
were recorded by an OIMS-500 Mössbauer spectrum instrument.
D
Eads ¼ EsurfþO ꢀ Esurf ꢀ EO
2
2
57Co (Pd) was used as a
was calibrated against standard
c
-ray radioactive source and the velocity
where EsurfþO ,Esurf , and EO represent the total energy of the
a-iron foil. N2 adsorption–
2
2
adsorbed oxygen molecules, the energy of the surface, and the
gas-phase energy of oxygen molecules, respectively.
desorption isotherms were measured at 77 K, using a Micromeritics
ASAP 2010 N analyzer. Samples were degassed at 423 K for 15 h
before measurements. Magnetic measurements were performed
on a vibrating sample magnetometer (YingPu VSM-400 Instru-
ments) at room temperature under an applied field of 40,000 Oe.
3. Results and discussion
3.1. Preparation and characterization of iron oxide catalysts
2.3. Catalytic test
Considering potential applications, three readily available and
A mixture of benzyl alcohol (1 mmol), aniline (2 mmol), catalyst
(0.3 g), and toluene (10 mL) was added into a 50-mL two-neck
stable iron oxides, hematite (
a-Fe2O3), magnetite (Fe3O4), and
maghemite -Fe2O3), were synthesized and systematically
(c