Co NMR studies have been performed in metallic NaCo 2 O 4 in the temperature range 350-100 K. The powder patterns predominantly correspond to typical second-order quadrupolar splitted central transition of two inequivalent cobalt sites. Features of magnetic interaction are also present. The analysis of the NMR line shape shows that the electric field gradient ͑EFG͒ experienced by one of the two sites ͑site 1͒ is independent of temperature, whereas around 47% increment in EFG has been observed for site 2 as the temperature is lowered from 350 to 100 K. 59 Co NMR shift for each site is almost isotropic in character which varies linearly with susceptibility and basically consists of two parts. Both the sites suffer a large temperature independent shift due to the contribution from orbital paramagnetism ( vv ) which is analogous in metals to the Van Vleck paramagnetic susceptibility. The temperature-dependent Knight shift for site 1 reveals a negative hyperfine coupling constant (A hf d ) arising from inner s core polarization by the d electrons which are itinerant in character. A positive A hf d observed for site 2 cannot be interpreted directly in a metallic system such as NaCo 2 O 4 . A comparison of the magnitude of A hf d with those of other cobalt oxides suggests that the nucleus which is being probed by NMR, belongs to a diamagnetic cobalt state. Thus the present NMR results together with the susceptibility indicate the presence of Co 3ϩ ion with S ϭ 0 and the magnetic Co 4ϩ ion.
Thermal conductivity of a 300-nm-thick VO 2 thin film and its temperature dependence across the metal-insulator phase transition (T MIT ) were studied using a pulsed light heating thermoreflectance technique. The VO 2 and Mo/VO 2 /Mo films with a VO 2 thickness of 300 nm were prepared on quartz glass substrates: the former was used for the characterization of electrical properties, and the latter was used for the thermal conductivity measurement. The VO 2 films were deposited by reactive rf magnetron sputtering using a V 2 O 3 target and an Ar-O 2 mixture gas at 645 K. The VO 2 films consisted of single phase VO 2 as confirmed by X-ray diffraction and electron beam diffraction. With increased temperature, the electrical resistivity of the VO 2 film decreased abruptly from 6.3 ' 10 %1 to 5.3 ' 10 %4 Ω cm across the T MIT of around 325-340 K. The thermal conductivity of the VO 2 film increased from 3.6 to 5.4 W m %1 K %1 across the T MIT . This discontinuity and temperature dependence of thermal conductivity can be explained by the phonon heat conduction and the Wiedemann-Franz law.
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