Ca2p3/2 and Ca2p1/2 states. These peaks are characteristics of Ca2+ ions in oxide environment
[43-47]. However, unlike pure CaO, where a well-defined valley is observed between the two
peaks, in this study these two peaks are broad and unresolved from one another. This may be due
to the fact that a small fraction of Ca2+ may exist in carbonate environment [44,45]. The CaCO3
show Ca2p doublet at 347.4 and 351.0 eV. The presence of Ca2+ ions in the solid solution phase
and a small fraction as surface carbonate species can be inferred from the XPS study.
The Raman spectra of the xCa-Zr-O composite materials along with pure ZrO2 are presented in
Fig. 6. The Raman technique is an effective method for microstructural analysis of crystalline
oxide phases. Particularly, the Raman technique has been highly effective for characterization of
different polymorphic forms of zirconia in composite materials [22,48, 49]. Pure ZrO2 prepared by
urea hydrolysis method exhibit intense Raman bands with maxima at 177, 187, 220, 331, 381, 500,
536, 559 and 615 cm-1 corresponding to the monoclinic phase and 146, 269,314, 475 and 638 cm-
1corresponding to the tetragonal phase of zirconia [22, 49]. In contrast to this observation, the xCa-
Zr-O composite oxide exhibit broad, asymmetric and low intense Raman bands corresponding to
the t-ZrO2 only [16,22]. The broadening of the peaks may be ascribed to the presence of large
amount of oxygen vacancy created due to incorporation of Ca2+ ions into the ZrO2 lattice [16,22].
Tetragonal zirconia belongs to P42/nmc space group and is expected to exhibit six Raman active
vibration modes having A1g + 3Eg + 2B1g symmetry [48,49]. Among these vibrational modes, the
symmetric A1g vibration appears around 600 cm-1 and is often too weak to be observed. In the
present study for the xCa-Zr-O composite, the broad Raman bands observed at 146 and 318 cm-1
can be assigned to 2 B1g modes and the bands at 269, 456 and 642 cm-1to the 3Eg modes,
respectively. The asymmetric nature of the Raman bands indicates distortion in the oxygen sub-
lattice caused by the insertion of the Ca2+ ions into the zirconia lattice.
The surface basic property of the xCa-Zr-O composite materials was studied using the CO2-TPD
technique. The TPD profiles of the xCa-Zr-O composite materials are presented in Fig.7. The TPD
profiles for the composite oxides contain three CO2 desorption regions in the temperature range of
< 400 K, 450-750 K and >750 K. Pure ZrO2 prepared by urea hydrolysis method exhibit
significant CO2 desorption below 400 K (Fig. 7a). This low temperature TPD peak can be assigned
to the presence of weak basic sites on zirconia surface. The addition of Ca2+ ions into the zirconia
lattice improves the CO2 retention at high temperature indicating generation of new basic sites of
higher strength (Fig. 7 b-e). For the 5Ca-Zr-O, 10Ca-Zr-O and 20Ca-Zr-O materials a strong CO2
desorption peak is noticed in the range of 400-750 K. Simultaneously, the low temperature
desorption peak below 400 K is significantly suppressed. With increase in Ca2+ content in the
composite, the high temperature TPD peak progressively shifts towards the higher temperature
side. For 50Ca-Zr-O material, a single prominent desorption peak is observed with peak maxima at
790 K (Fig, 7e). The CO2-TPD method has been used earlier for characterization of basic sites of
CaO-ZrO2 composite materials. The basicity of the CaO-ZrO2 material depends on various factors
such as the preparation method, the crystallographic phase of zirconia, CaO content and
calcinations temperature [11, 15-18, 22]. The tetragonal phase of zirconia and a higher calcination
temperature facilitates the incorporation of Ca2+ ions into the zirconia lattice [18,22]. The presence
of Ca2+ ions in the vicinity of O2- ions improves the basicity of the lattice oxygen on the surface.
Moreover, the incorporation of Ca2+ to ZrO2 lattice leads to the formation of Ca-O-Zr linkages and
uneven charge distribution which is responsible for generation of new basic sites [13]. In the
present study, the desorption peak in the temperature range of 450-750 K can be assigned to the
generation of new basic sites due to solid solution formation. The TPD peak observed at 790 K for
50Ca-Zr-O material can be ascribed to the formation of CaO crystallites which has been detected
7