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812
Communications of the American Ceramic Society
Vol. 87, No. 9
Fig. 3. XPS spectra of the as-prepared ␣-Si N powders.
3
4
about 75 mL in capacity was sealed under an argon atmosphere
and maintained at 450°, 500°, 550°, and 600°C (Ϯ 5°C) for
the wide-scan XPS spectrum except a small amount of carbon
(reference mark) and oxygen, with binding energies of C1s and
O1s at 284.26 and 531.95 eV, respectively, in which oxygen is
1
0 h. The autoclave was cooled to room temperature naturally.
1
6
The products were collected and washed with distilled water
several times to remove MgCl and remaining NH Cl. The final
from surface adsorption.
According to the free energy calculations, the reaction between
2
4
products were dried in vacuum at 70°C for 12 h and white
powder products were obtained.
Mg Si and NH Cl to form ␣-Si N , MgCl , NH , and hydrogen
2
4
3
4
2
3
o
gases is thermodynamically spontaneous (calculated ⌬G ϭ Ϫ400
Ϫ1 o
kcal⅐mol ) and mildly exothermic (calculated ⌬H ϭ Ϫ227
Ϫ1
kcal⅐mol ). A gust of gases with an ammonia smell were noticed
III. Results and Discussion
when the autoclave was unsealed. An approximately stoichiomet-
ric amount of Mg(OH) according to the amounts of Mg Si was
2
2
The X-ray diffraction (XRD) patterns were recorded on an
X-ray diffractometer (XRD)(D/MAX-␥A, Rigaku, Japan) with Cu
K␣ radiation (wavelength ϭ 1.54178 ⌭). Figure 1 shows the
XRD patterns of the as-prepared products at 350°–600°C. As
shown in Table I, all the 26 peaks can be indexed as the hexagonal
cell of ␣-Si N , with lattice constants of a ϭ 7.770 and c ϭ 5.627
obtained by treating the water used to wash products with NaOH.
The maximal pressure is about 30 to 40 MPa in the temperature
range of 450° to 600°C, which is estimated according to the
amount of NH and hydrogen treated as ideal gases. Varying the
3
reaction temperature in the range of 450°–600°C did not signifi-
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4
cantly affect the crystallinity or the yields of Si N (about 93%
Ϫ4
3 4
Å (The rms error is 3.153 ϫ 10 , calculated by the least squares
fitting method), in good agreement with a ϭ 7.765 and c ϭ 5.627
Å (JCPDS card# 83–0700). No evidence of -Si N , cubic-Si N ,
according to the amount of Mg Si). In comparison, polycrystalline
2
silicon powders were found unreacted and Si N was not produced
3
4
3
4
3 4
when excessive NH Cl and mixed powders of magnesium and
4
and impurities were observed. As reaction temperatures decrease
from 600° to 450°C, the diffraction peaks broaden, indicating the
crystalline particles of the products become smaller.
silicon were heated at 600°C for 10 h in an autoclave. A mixture
of amorphous Si N and polycrystalline silicon was produced
3
4
when CaSi (Alfa Aesar, stock #14676) was heated with excessive
2
The morphology of the ␣-Si N powders was investigated by
3
4
NH Cl at 600°C for 10 h in an autoclave. When FeSi powders
4
transmission electron microscopy (TEM) (H-800, Hitachi, Japan),
which was taken with a Hitachi H-800 transmission electron
microscope. Figure 3 shows the typical TEM images and selected
area electron diffraction (SAED) patterns of the samples prepared
at 450°, 500°, and 550°C for 10 h. The products have particle
morphology. The ␣-Si N crystallites prepared in 450° (Fig. 3(a)
(
primitive cubic phase, a ϭ 4.415 Å, prepared by the reaction of
17
FeCl and Mg Si at 600°C for 12 h ) were used instead of Mg Si,
3
2
2
Si N was not produced and the FeSi remained unreacted, indi-
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4
cating that Mg Si is the key factor for preparing nanocrystalline
2
␣
-Si N at the low temperature range of 450° to 600°C.
3 4
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4
and (b)), 500° (Fig. 3(c)), 550° (Fig. 3(d)), and 600°C (not
published) are about 20, 40, 70, and 90 nm in average, respec-
tively. As shown in Fig. 3(b), the diffraction rings from inner to
outer, at d-spacings of 6.70, 4.29, 2.90, 2.60, 2.54, and 2.30 Å,
match ␣-Si N (100), (101), (201), (102), (210) and (Ϫ2–11)
IV. Conclusions
In summary, about 20- to 90-nm ␣-Si N powders have been
3
4
prepared by the reaction of Mg Si with NH Cl in the temperature
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4
3
4
range of 450° to 600°C in an autoclave. XRD patterns of the
products can be indexed as ␣-Si N with the lattice constants of
planes, in good agreement with the XRD results.
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4
The composition of the as-prepared ␣-Si N powders was
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4
a ϭ 7.770 and c ϭ 5.627 Å. XPS analysis indicates that the
composition of the ␣-Si N samples has a Si:N ratio of 0.756.
studied by X-ray photoelectron spectroscopy (XPS) (ESCALAB
MKII, VG Scientific, U.K.), which was recorded on a VGES-
CALAB MKII X-ray photoelectron spectrometer with a non-
monochromatized Mg K␣ X-rays (h␥ ϭ 1253.6 eV) as the
excitation source. As shown in Fig. 2, the binding energy of Si2p
and N1s are 101.70 and 397.75 eV, respectively, which are in good
agreement with those of Si N (101.7–102.34 eV and 397.4–397.9
3
4
Such nanocrystalline ␣-Si N powders hold great potential for
3
4
improving properties of ceramic structural materials. This study
demonstrates an important route to nanocrystalline ␣-Si N that
3
4
can be applied for industrial use in the future.
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4
1
1,12,13,14,15
References
eV, respectively
). The quantification of the peaks gives
a Si:N ratio of 0.756, which is close to that of Si N (0.750). In
1
3
4
3 4
F. Rodriguezreinoso and J. Narciso, “Synthesis of SiC and Si N –An Overview,”
addition to silicon and nitrogen, no other peaks were observed in
Adv. Mater., 7 [2] 209–11 (1995).