Cobalt Molybdenum Nitrides
J. Phys. Chem. B, Vol. 105, No. 19, 2001 4085
at 773 K for 7 h in dry air. The precursors were placed on a
fritted quartz plate in a 10 mm i.d. quartz microreactor and then
nitrided by a temperature-programmed reaction (TPR) with
ammonia (99.99%). A 0.2 g sample was oxidized in dry air
and mortar, dispersed in ethanol with an ultrasonic apparatus,
placed on a copper microgrid, and transferred to the analysis
chamber in the TEM.
XPS and Elemental Analysis. X-ray photoelectron spec-
troscopy was carried out using a Shimadzu ESCA 3200
photoelectron spectrometer with Mg KR radiation (1253.6 eV,
-
1
(
1.11 mL s ) at 723 K for 1 h for an oxidized sample. For
nitrided samples, the 0.2 g sample was oxidized in dry air at
23 K for 1 h, cooled from 723 to 573 K in dry air, nitrided
7
8
kV, 30 mA). The samples after nitriding were removed from
-
1
-1
from 573 to 973 K at a rate of 0.0167 K s with 1.11 mL s
the microreactor and then transferred to a glovebag in which
the atmosphere was exchanged with argon (99.9999%) five
times and filled with argon gas. The samples were mounted on
a holder with carbon tape in the glovebag without exposure to
air. Argon etching was done for the analysis of the bulk samples
of ammonia, held at this temperature for 3 h, and then cooled
to room temperature in flowing ammonia. The other oxidic
precursor was prepared from a physical mixture of CoO and
MoO3 (Co/(Co + Mo)) ) 0.5, after nitriding the sample for
comparison. To compare the catalytic properties of the nitrided
catalysts with the sulfided catalyst, Co(25) was sulfided at 623
-4
at a pressure of 8 × 10 Pa for 1 min. The analysis was
-6
typically done at a pressure of 5 × 10 Pa and at a scan speed
-
1
K under a stream of 10% H2S/H2 (4 L h ) after the catalyst
was heated at 723 K in air. The sample names of the cobalt
-1
-1
of 0.33 eV s with 0.05 eV (step) . The binding energy of C
1
s (284.6 eV) was taken as a reference to correct the binding
-
2
molybdenum samples are abbreviated Co(x)y, where x × 10
energy of the samples. The envelopes of the XPS binding
energies of Mo 3d, Mo 3p, Co 2p, and N 1s were deconvoluted
using Origin package software (Microcal Co.) after the analytical
data were transferred from the Shimadzu ESCA 3200 to a PC
data station. Since the binding energies of XPS Mo 3d3/2 and
is the atomic ratio of Co/(Co + Mo) in the oxides and nitrides
and y is 723 K for oxidizing or is 773-1073 K for the nitriding.
For example, Co(20)723 denotes the cobalt molybdenum
samples (Co(NO3)2‚H2O and (NH4)6Mo7O24‚4H2O with Co/(Co
Mo) ) 0.2) oxidized at 723 K. Co(50)973 and Co(5-25)-
73 denote the cobalt molybdenum samples with Co/(Co + Mo)
0.5 and 0.05-0.25, respectively, nitrided with ammonia at
BET Surface Area. The specific surface areas of the samples
+
9
)
0
2+
3+
3
d5/2 and Co 2p3/2 and 2p1/2 had many peaks (Mo , Mo , Mo ,
4+
5+
6+
0
2+
3+
Mo , Mo , and Mo and Co , Co , and Co ), the binding
energies and fwhms of Mo 3d and Co 2p were fixed and
9
73 K.
0
deconvoluted, except for those of Co (-0.5 to 0.5 eV deviation
from the binding energy of Co0 at 777.6 eV). The spectra of
XPS Mo 3d of the cobalt molybdenum nitrided samples were
were measured using an Omnisorp 100CX (Beckman Coulter
Co.). The surface area of the samples (0.1 g) was measured by
nitrogen adsorption at liquid-nitrogen temperature after the
deconvoluted using an intensity ratio of 2/3 and a splitting of
34
3
.2 eV and referenced to the data reported by Hercules et al.
-
4
sample was evacuated at 473 K and 1.3 × 10 Pa for 2 h.
35
0
and Hada et al.: Mo (Mo 3d5/2 binding energy, 227.7 ( 0.2;
2+
3+
XRD. The sample before and after nitriding was measured
fwhm, 1.2 ( 0.2), Mo (228.4 ( 0.1; 1.4 ( 0.2), Mo (229.2
4
+
5+
by XRD. The nitrided sample was passivated in 1% O2/He
( 0.1; 1.5 ( 0.3), Mo (230.1; 1.6 ( 0.2), Mo (231.6; 1.65
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1
6+
(
0.167 mL s ) for longer than 12 h at room temperature after
nitriding. The diffraction pattern was obtained using a RAD-II
Rigaku Co.) equipped with Cu KR radiation (λ ) 1.542 Å).
( 0.2), and Mo (233.0; 1.7 ( 0.2). Since the Co 2p spectra
were very broad and difficult to deconvolute for both Co 2p3/2
0
2+
(
and 2p1/2 in the region of 775-805 eV, the peaks of Co , Co ,
3+
2+
The peaks were identified on the basis of the JCPDS card
references: MoO3 (JCPDS 5-0508, 2θ ) 12.8, 25.7, and 27.4°;
this study, 2θ ) 12.9, 25.8, and 27.4°), MoO2 (JCPDS 32-671,
Co , and Co satellites were fitted for only the Co 2p3/2 region
for all the samples. The peak fittings of the XPS Co 2p3/2 binding
energies were referenced to the data of cobalt molybdenum
3
6
2
5
θ ) 26.1, 36.9, and 53.2°; this study, 2θ ) 26.0, 36.9, and
3.6°), γ-Mo2N (JCPDS 25-1366, 2θ ) 37.4, 43.5, and 63.2°;
2 3
sulfides obtained by Pawelec et al., of CuCo/Al O by
Figueiredo et al., and of Co/Al O by Zsoldos et al. The Co
3
7
38
2
3
this study, 2θ ) 37.3, 43.5, and 63.0°), CoO (JCPDS 43-1004,
2p3/2 binding energies for the cobalt molybdenum nitrided
0
2
6
θ ) 36.5, 42.4, and 61.6°; this study, 2θ ) 36.7, 42.3, and
1.4°), Co metal (JCPDS 15-806, 2θ ) 44.8, 47.6, and 76.0°;
samples were deconvoluted to Co (BE, 777.6 ( 0.8 eV; fwhm,
2
+
3+
1.3 ( 0.1 eV), Co (779.9 ( 0.4 eV; 4.2 eV), Co (781.6 (
2
+
this study, 2θ ) 44.8, 47.5, and 75.9°), and CoMoO4 (JCPDS
0.3 eV; 4.7 ( 0.1 eV), and Co satellite (786.1 ( 0.3; 5.0
eV). The base line corrections made of the peak fitting of Co
2p3/2 and Mo 3d were carried out with the Shirley method
provided by the Shimadzu spectrometer manufacturer. Further-
more, the XPS N 1s binding energy of the samples at 397 (
0.3 eV (fwhm 2.0 eV) was used to calculate the nitrogen content
in the samples on the basis of a new determination method39
for the deconvolution of Mo 3p3/2 and N 1s in the region of
390 and 410 eV. Elemental analysis of the samples was carried
out using a Shimadzu CHN 123 elemental analyzer (oxygen
burning method) after the samples were evacuated at 673 K
2
)
1-868 and 25-1434, 2θ ) 14.2, 26.7, and 28.5°; this study, 2θ
14.2, 26.5, and 28.5°). The peaks of cobalt molybdenum
25
nitride were consistent with the data reported by Jackson et al.
and Kim et al.22 such that Co3Mo3N had peaks at 2θ ) 40.0,
4
2.6, 46.6 and 72.8°. The peaks of Co-Mo oxynitride were
identified by comparison with the data reported by Oyama and
2
3
co-workers at the broad peaks of 2θ ) 37.0, 43.0, and 63.0°.
Temperature-Programmed Reaction with NH3 (TPR). The
oxidic precursor after oxidizing at 723 K was heated from 573
-
1
-1
to 973 K at a rate of 0.167 K s with 1.11 mL s of ammonia
99.99%). The desorbed gases were monitored using a Balzers
-
4
(
and 1.3 × 10 Pa for 2 h.
Quadstar 422 quadrupole mass spectrometer. Ammonia and
water in the desorbing gases during TPR were qualitatively
analyzed at m/z 15 and 18, respectively, because they overlapped
at m/z 17. Hydrogen and nitrogen were monitored at m/z 2 and
HDS of Thiophene. The flow system for the HDS of
40
thiophene is described elsewhere. The system consisted of a
single-pass, differential microreactor. The HDS of thiophene
on the nitride and sulfide catalysts (ca. 0.2 g) were carried out
at 623 K and atmospheric pressure. The reaction feed, consisting
of 3.8 vol % thiophene in pure hydrogen, was introduced at a
2
8, respectively.
TEM. The morphology of the samples was determined using
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1
a JEM-2000F transmission electron microscope (JEOL Co.)
operating at 200 kV equipped with an energy-dispersive X-ray
spectrometer (EDS). The sample was crushed in an agate pestle
rate of 50 mL min into the reactor. Quantitative analysis was
performed by injecting a sample from a sampling loop into the
gas chromatograph to analyze the amount of thiophene (column