6850
R. Dwivedi et al. / Journal of Alloys and Compounds 509 (2011) 6848–6851
0.8
0.7
0.6
0.5
0.4
50000
2355
ZrO2
(A) ZrO2 , 600°C
(B) ZrO2 , 800°C
2323
40000
1554
30000
1523
123
146
20000
259
470
382
10000
0
643
(A)
(B)
0
1000
2000
Cm-1
3000
2000
Cm-1
1000
Fig. 4. Raman spectra of ZrO2 precipitated at pH 2 and calcined at different temper-
atures.
Fig. 3. FTIR spectrum of ZrO2 in the range of 3500–500 cm−1
.
modes on the simple reasoning that these two modes also does not
involve movement of Zr atoms. The remaining three modes namely
two B1g modes and one Eg mode are assigned to the remaining three
band appearing at 259, 146 and 123 cm−1, respectively. The spec-
trum of sample calcined at 600 ◦C is shown as curve (B) in Fig. 4. The
above bands appeared in the Raman spectra for both the samples
are assigned to t-ZrO2. In addition, few faint bands at 563, 536, 381,
293, 176 cm−1 have appeared which are due to the co-existence of
small amount of monoclinic phase.
the spacing of (1 0 1) planes of the t-ZrO2. The corresponding SAD
pattern is inserted into the micrograph. The clear spots in SAD pat-
tern suggest that the crystallites are of sufficiently large size. The
absence of rings in the SAD pattern is indicative of the crystalline
order, larger particle size and long-range order in the crystallites.
The TEM results also suggest the successful preparation of tetrag-
onal phase of ZrO2 nanocrystals with the crystallite sizes ranging
∼5–10 nm.
BET surface area was measured for the prepared zirconia sam-
ples calcined at 450 ◦C for 4 h. The average values calculated for
surface area was 38.7767 m2/g and pore size was 3.85247 nm.
FTIR spectra of the samples in the range 400–4000 cm−1 were
recorded. Fig. 3 shows the FTIR spectrum for the zirconia nanopar-
ticles in absorbance mode. The prominent band at 2355 cm−1 and
2323 cm−1 corresponds the structural O–H stretching of the nano-
materials. In the bending mode region two bands are observed at
1554 cm−1 and 1523 cm−1, which are due to the O–H bending. In
addition the broad band at 900–1000 cm−1 can be assigned to the
Zr–O bond for t-ZrO2.
Raman spectroscopy is sensitive to the polarizability of the oxy-
gen ions and therefore it can be used to determine the symmetry
sensitive to short-range order than X-ray diffraction, and it can
show the peaks for anatase or rutile as well as monoclinic zirco-
ZrO2 calcined at the temperatures of 600 ◦C and 800 ◦C are plot-
ted in Fig. 4. The assignment of the observed bands was made on
the basis of the comparison of the observed spectra with that of
reported in the literature [24,25,30]. The vibrational Raman active
modes are classified as:
4. Conclusions
Zirconia nanoparticles were synthesized by the simple and most
convenient microware assisted citrate sol–gel method. The for-
mation of tetragonal crystalline phase t-ZrO2 was confirmed by
powder XRD analysis on calcined samples. The morphology, par-
ticle size and microstructure were analyzed using high-resolution
transmission electron microscopy. The HRTEM data also confirms
the formation of single phase t-ZrO2. The high-resolution TEM
micrograph and SAD pattern show the crystalline perfection and
long-range order in the prepared zirconia nanoparticles. The crys-
tallite sizes were found in the range of ∼5–10 nm. Raman spectra
further supports and confirms the crystalline phase as well as the
specific bands to show the modes of vibration in Zr–O system.
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modesalsoinvolve motionin the z-direction, howevernow ZrandO
in the x–y plane. Pictorial description of the modes can be found
elsewhere [31]. Fig. 4 shows the Raman spectra of ZrO2 nanoparti-
cles precipitated at pH 2 and calcined at different temperatures.
Fig. 4(A) represents the Raman spectra for the sample calcined
at 400 ◦C. The band appeared at 643 cm−1 can be assigned to A1g
mode since it involves movement of two oxygen atoms only and
is expected to appear at higher wave number. The next two bands
appeared at 470 and 382 cm−1 are assigned to doubly degenerate Eg