Abstract:Differently heat‐treated polycrystalline cadmium oxide (CdO) samples have been studied using room temperature (RT) resistivity, positron annihilation lifetime (PAL) and ultraviolet visible (UV‐Vis) optical absorption measurements. A small increase of the resistivity for 275 °C annealing (with respect to the other samples) and a large reduction of the same for 810 °C annealing have been observed. PAL investigation shows presence of defects, presumably Cd+O divacancy (VCd+O) clusters, in all the samples. Gradual… Show more
“…Positrons experience a relatively lower electron density on the nanocrystallite surfaces and hence will have larger lifetimes. In our previous work [37], we had reported the positron lifetimes in two samples of CdO with I 2 < 2% and the corresponding τ 1 (= 0.135 ns) had been accepted as the lifetime of positrons in bulk CdO, consistent with the value reported by others in literature [43]. The effect of contraction of the lattice of the Zn-doped samples on the bulk lifetime is quantitatively estimated using the method proposed by de la Cruz et al [44].…”
Pure and zinc-doped cadmium oxide nanocrystallites of sizes in the range 25 nm to 16 nm are synthesized by adopting a chemical precipitation method and by varying the doping concentration from 0.0 to 0.25 at.%. The decrease in nanocrystallite sizes with increasing substitution is expected from the smaller ionic radii of Zn2+. But more revealing is the interfacial defects formation at higher concentration of doping, which is attributed to the dissimilar crystalline structure of ZnO and CdO. X-ray diffraction patterns show well defined peaks and additional characterisation is done through transmission electron microscopy. The optical band gap measurements indicate the dominance of substitution-induced disorder over the confinement of excitons, leading to a decrease in the band gap energies. The results of positron annihilation studies confirm the cancellation of the existing vacancy type defects in the initial stage, followed by the substitution. Photoluminescence spectra reveal the distinct peaks of optical plasmonic excitations and the defect population in the bandgap and the intensity variations agreed with that of the defect related positron annihilation intensity. The segregation of ZnO phase leading to the formation of interfacial boundaries is found as a strong deterrent against the success of continued substitution.
“…Positrons experience a relatively lower electron density on the nanocrystallite surfaces and hence will have larger lifetimes. In our previous work [37], we had reported the positron lifetimes in two samples of CdO with I 2 < 2% and the corresponding τ 1 (= 0.135 ns) had been accepted as the lifetime of positrons in bulk CdO, consistent with the value reported by others in literature [43]. The effect of contraction of the lattice of the Zn-doped samples on the bulk lifetime is quantitatively estimated using the method proposed by de la Cruz et al [44].…”
Pure and zinc-doped cadmium oxide nanocrystallites of sizes in the range 25 nm to 16 nm are synthesized by adopting a chemical precipitation method and by varying the doping concentration from 0.0 to 0.25 at.%. The decrease in nanocrystallite sizes with increasing substitution is expected from the smaller ionic radii of Zn2+. But more revealing is the interfacial defects formation at higher concentration of doping, which is attributed to the dissimilar crystalline structure of ZnO and CdO. X-ray diffraction patterns show well defined peaks and additional characterisation is done through transmission electron microscopy. The optical band gap measurements indicate the dominance of substitution-induced disorder over the confinement of excitons, leading to a decrease in the band gap energies. The results of positron annihilation studies confirm the cancellation of the existing vacancy type defects in the initial stage, followed by the substitution. Photoluminescence spectra reveal the distinct peaks of optical plasmonic excitations and the defect population in the bandgap and the intensity variations agreed with that of the defect related positron annihilation intensity. The segregation of ZnO phase leading to the formation of interfacial boundaries is found as a strong deterrent against the success of continued substitution.
“…However, current decade finds use of these oxide semiconductors, with potential application in optoelectronics and high-performance electronic device applications. While ZnO, with 3.3 eV room-temperature band gap (Eg) and large exciton binding energy of 60meV, is playing the main role in many II-VI optoelectronic devices, their spectral range is being extended [3] into the visible and deep ultraviolet ranges by alloying ZnO with the smaller band-gap compound CdO [4], having room-temperature E g of ~2.2eV at the Brillouin-zone centre, and with larger band-gap compound MgO [3,5] with E g of 7.7eV, respectively. We find non-stoichiometry [6][7][8][9][10] and, hence, widely varying electrical conductivity [2] in differently heat-treated cadmium ox ide (Figure 1).…”
Section: Introductionmentioning
confidence: 99%
“…Room temperature resistivity of as-supplied E Mark (India) cadmium oxide was 97m Ωcm. Firing [4,7] at 270 °C reduce it to ~26.4 m Ω cm. Resistivity reduces, further, to ~2.1 m Ω cm after 800 °C heat treatment.…”
Section: Introductionmentioning
confidence: 99%
“…However, even the pure material is complex, exhibiting non-stoichiometry and defect structures, as a function of its preparation or heat treatment temperature. Positron annihilation spectroscopy (PAS) being a powerful tool to study defects in soft [14] and hard [4,15] condensed matter, we investigate silicone-rubber CdO complex samples by positron lifetime spectroscopy (PLS) [14,15]. There are still a few poorly understood aspects of cadmium oxide like its non-stoichiometry (Figure 2) and colour, although cadmium oxide has been well investigated experimentally and theoretically for many decades.…”
Cadmium oxide (CdO) exhibit altered properties with altered Cd: O composition after heat treatment at different temperatures. This has been probed experimentally by various techniques. High electrical conductivity (low resistivity of ~2m Ωcm) after 800 °C firing has inspired novel applications, in many of which the brittleness of the fired ceramic become a bottleneck. Here, flexible composites of these fired cadmium oxides have been formed with a silicone rubber binder and tested with respect to properties like carrier concentration and fractional free volume by positron lifetime spectroscopy. Fractional free volume, V f , 15.32% in the pure silicone rubber, reduces to 9.40% for the composite with 59.13 wt% of 800 °C fired cadmium oxide. Bulk lifetime τ B for positrons in a sample is shorter for higher number density of electrons in the bulk. It reduces from 203.78ps for pure silicone rubber, to 174.01ps for the same composite.
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