Y.-J. Hsiao et al. / Journal of Alloys and Compounds 475 (2009) 698–701
699
Fig. 1. DTA and TG curves for CaNb2O6 precursor.
3. Results and discussion
The TG and DTA curves of the dry CaNb O precursor are shown
2
6
◦
in Fig. 1. The endothermic peak at about 110 C in DTA accounted
for 10% of the initial weight loss in TG, was assigned to the loss of
ethanol and free water. A fast weight loss stage of about 46% in the
Fig. 2. X-ray diffraction patterns of CaNb2O6 precursor powders annealed at (a) 500,
(b) 600 and (c) 700 C for 3 h.
◦
◦
range of 110–400 C that was accompanied by one exothermic peak
peak angle, and ˇ is half the peak width. The average grain sizes
◦
◦
at 370 C. The exothermic peak at 370 C was due to the burnout
of the low boiling organic species and the other exothermic peak
originated from the burnout of the organic groups in citric acid. In
◦
of powders calcined at 600 and 700 C were about 22.3 and
2
8.6 nm, respectively. The particle size increased as the sintering
temperature was increased. It is believed that a higher temper-
ature enhanced higher atomic mobility and caused faster grain
growth.
◦
addition, a manifest exothermic peak around 610 C, that was asso-
ciated with the decomposition the amorphous gel into main phase
CaNb O . In this experiment, the possible chemical reactions for
2
6
TEM analysis of the crystal provided further insight into the
the synthesis of CaNb O6 powders can be expressed as following:
◦
2
structural properties of as-synthesized CaNb O6 at 700 C. Fig. 3a
2
showed the low-magnification TEM image, and the morphology
was clearly observed. The big particles were condensed by assem-
bled nanograins. It was conjectured that the assemble effect arising
from nanocrystals, are responsible for the decreasing of surface
energy. There was only one orthorhombic crystalline phase exist-
ing in the ceramic matrix. The well-defined selected area electron
diffraction (SAED) pattern clearly shows the diffraction spots in
Fig. 3b, that was calculated the inter-planar spacing of the diffrac-
tion spots in patterns and the experimental d values well-fitted the
JCPDS card. The EDS results confirmed the composition with Ca and
Nb ion content and the molar ratio of Ca to Nb almost about 0.5 in
Fig. 3c.
CA
Ca(NO ) + 2Nb(OC H5) −→ CaNb O + NO ↑ +H O ↑ +CO2
↑
3
2
2
5
2
6
2
2
+C2H5OH ↑
(2)
◦
Therefore, the weight loss between 110 and 610 C in the TG
curve was caused by the generation of organic groups and many
kinds of gas from the precursor.
The amorphous metal-organic gel was heat-treated to pyrolyze
the organic components for crystallization. XRD patterns of the
precursor powders at heat-treatment temperatures of 500–700 C
for 3 h are shown in Fig. 2. Calcined temperatures at 500 C had
shown almost amorphous phases. The content of CaNb O phase
had a rapid product at 600 C that is due to decompose amor-
phous gel. When the precursor sintered at temperatures 700 C,
◦
◦
2
6
Fig. 4 presents the excitation spectra of the CaNb O sam-
2 6
◦
◦
ples at temperatures of 600 and 700 C. The photoluminescence
results reveal that the sample prepared at 700 C exhibits greater
◦
◦
the samples exhibited a single phase and all of the peaks were
absorption intensity at 257 nm than other samples by monitoring
fluorescence at a wavelength of 457 nm. Blasse [15] indicated that
identified to be the orthorhombic CaNb O6 phase (JCPDS file
2
7
−
the niobate complexes had two kinds of absorbing groups [NbO ]
6
No. 71-2406). Note that the intensity of the diffraction peaks
becomes sharper at higher temperatures, indicating that the
and [NbO4]3 , respectively. Only one peak was observed at wave-
−
◦
crystallinity of CaNb O6 increases with the increase of the cal-
lengths of 257 nm, as the calcining temperature at 600 and 700 C.
2
cination temperature. The average grain sizes were determined
from XRD powder pattern according to the Scherrer’s equation
Therefore, the peaks of excitation, at about 257 nm, were associated
with charge transfer bands of [NbO6]7 in the CaNb O system. The
−
2
6
[
14],
crystal structure of CaNb O was described as a layer structure built
2 6
up by edge-sharing of NbO6 trigonal prisms [16].
kꢀ
D =
(3)
The PL emission spectral wavelength distribution curves of
ˇ cos ꢁ
CaNb O6 phosphors under 257 nm excitation at room tempera-
2
where D is the average grain size, k is a constant equal to 0.89,
is the X-ray wavelength equal to 0.1542 nm, ꢁ is the (3 1 1)
ture are shown in Fig. 4. The PL spectra show a broad and strong
blue emission peaks at about 457 nm. Here, the edge-shared NbO6
ꢀ