Communications
Magnetic measurements were carried out in a Quantum-Design
SQUID magnetometer; magnetization isotherms were collected at 4
and 300 K between À50 kOe and + 50 kOe. Photoelectron spectra
were recorded with a VG Escalab 200R electron spectrometer
provided with MgKa X-ray source and a hemispherical electron
analyzer. The binding energies were referenced to the C1s peak at
284.9 eV. Data processing was performed with the XPS peak
program, and the spectra were decomposed with the least-squares
fitting routine provided with the software with Gaussian/Lorentzian
(90/10) lines and after subtracting a Shirley background.
Table 2: Products of the oxidation of alkyl aromatics at 20 bar O2 after
3 h of reaction over NHPI/(La,Sr)0.5(Mn,Co)0.5O3Àδ
.
Substrate
Conv. [%]
Product
distribution [%]
99.7
98.1
63.0
1.9
The oxidation of alkyl aromatics was performed in a 100 mL steel
autoclave (autoclave Engineers). In a typical run, 1.46 g of substrate,
0.435 g of N-hydroxyphthalimide, 50 mg of perovskite or 0.0166 g of
cobalt(II) acetate, 0.0115 g of manganese(II) acetate, and 20 mL of
acetic acid were mixed together. The reactor was pressurized with
oxygen at 20 bar and the temperature was set to 363 K. Then, the
stirring was started and set at 1000 rpm. The pressure was maintained
at 20 bar, and fresh oxygen was fed in as it was consumed. The liquid
was analyzed by gas chromatography with a flame ionization detector
(GC-FID) on an Agilent 6850 device equipped with an HP-WAX
column. Crystallographic data for oxidized (La,Sr)0.5(Mn,Co)0.5O3:
99.8
100
37.0
ꢀ
R3c, hexagonal setting, a = 5.4463(5) ꢀ, c = 13.2885(2) ꢀ, V=
341.355(6) ꢀ3, O1 (x,0,1= ) x = 0.4745(1), 1calcd = 8.386 gcmÀ3, Z = 6,
4
R
wp = 3.19%, Rp = 2.42%, Rexptl = 1.95%, c2 = 2.68, RBragg = 2.55%,
99.1
0.9
measurement range 108 ꢀ 2q ꢀ 1608, 3198 data points, 80 observed
reflections, 68 parameters refined. Crystallographic data for reduced
(La,Sr)0.5(Mn,Co)0.5O3Àd at 423 K: Pbnm, a = 5.5071(4) ꢀ, b =
5.4873(5) ꢀ, c = 7.7898(6) ꢀ, V= 235.40(3) ꢀ3, 1calcd = 7.890 gcmÀ3
,
hypostoichiometric material shows an extraordinary reaction
rate and selectivity for the conversion of alkyl aromatics, for
example, p-xylene in TPA, with respect to the standard
homogeneous catalyst. The fact that this (La,Sr)0.5-
(Mn,Co)0.5O2.38 perovskite phase is ferromagnetic above
room temperature constitutes an added advantage, since it
could be separated from the solid product with a magnet; the
mother liquor could be removed by filtration to yield pure
TPA.
Z = 4, Rwp = 3.22%, Rp = 2.48%, Rexptl = 1.85%, c2 = 3.05, RBragg
=
8.38%, measurement range 108 ꢀ 2q ꢀ 1608, 3198 data points, 254
observed reflections, 23 parameters refined. Further details on the
crystal structure investigation may be obtained from the Fachinfor-
mationszentrum Karlsruhe, 76344 Eggenstein-Leopoldshafen, Ger-
many (fax: (+ 49)7247-808-666; e-mail: crysdata@fiz-karlsruhe.de),
on quoting the depository numbers CSD-422410 and -422411 for the
oxidized and reduced phases, respectively.
Received: December 15, 2010
Revised: April 13, 2011
Published online: May 31, 2011
Experimental Section
Keywords: heterogeneous catalysis · magnetic properties ·
neutron diffraction · oxidation · perovskite phases
The oxygen-stoichiometric (La,Sr)0.5(Mn,Co)0.5O3 oxide was obtained
by a nitrate–citrate route followed by a heat treatment at 11508C 12 h
in air. The subsequent reduction of the polycrystalline powder at
5208C for 8 h in H2/N2 (5%/95%) forming gas promotes the
formation of the extremely oxygen-defective (La,Sr)0.5(Mn,Co)0.5O2.38
perovskite. Thermal analysis was carried out in a Mettler TA3000
system equipped with a TC10 processor unit. Thermogravimetric
(TG) curves were obtained in a TG50 unit, working at a heating rate
of 108CminÀ1 in an H2/N2 (5%/95%) or O2 flow of 0.3 LminÀ1. The
initial characterization of the products was carried out by laboratory
X-ray diffraction (XRD) with a Bruker-axs D8 Advanced diffrac-
tometer (40 kV, 30 mA) with Cu Ka radiation (l = 1.5418 ꢀ) and a
PSD (position sensitive detector). The crystallographic structures of
the oxidized and reduced samples were refined from high-resolution
neutron powder diffraction (NPD) patterns collected at the Institut
Laue-Langevin (ILL) in Grenoble (France), acquired at 295 and
423 K at the D2B diffractometer with l = 1.594 ꢀ. The high-intensity
mode was used; the collection time was 2 h. The refinement of the
crystal structure was performed by the Rietveld method, using the
FULLPROF refinement program[22] and its internal tables for the
coherent scattering lengths of the corresponding elements. The peak
profiles were fitted by the Thompson–Cox–Hastings pseudo-Voigt
function corrected for axial divergence asymmetry. The following
parameters were refined in the final run: scale factor, background
coefficients, zero-point error, pseudo-Voigt corrected for asymmetry
parameters, positional coordinates, and anisotropic thermal factors.
.
[2] P. P. Toribio, J. M. Campos-Martin, J. L. G. Fierro, J. Mol. Catal.
A 2005, 227, 101.
[3] P. P. Toribio, J. M. Campos-Martin, J. L. G. Fierro, Appl. Catal. A
[4] L. Barrio, P. P. Toribio, J. M. Campos-Martin, J. L. G. Fierro,
[5] P. P. Toribio, A. Gimeno-Gargallo, M. C. Capel-Sanchez, M. P.
[9] H. Falcon, J. M. Campos-Martin, S. M. Al-Zahrani, J. L. G.
[10] R. A. Sheldon, I. W. C. E. Arends, J. Mol. Catal. A 2006, 251,
200.
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2011, 50, 6557 –6561