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Biennial Report 2005-2007 - Saha Institute of Nuclear Physics

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Condensed Matter <strong>Physics</strong> 109ing the coexistence <strong>of</strong> ferromagnetic and CO states. We have prepared nanocrystalline sample <strong>of</strong>Pri 0.65 (Ca 0.7 Sr 0.3 ) 0.35 MnO 3 , Pr 0.65 (Ca 0.6 Sr 0.4 ) 0.35 MnO 3 and Pr 0.65 (Ca 0.5 Sr 0.5 ) 0.35 MnO 3 . The studieson Pr 0.65 (Ca 0.6 Sr 0.4 ) 0.35 MnO 3 have indicated that the co-existence <strong>of</strong> CO and metallic stateexists. The insulator to metal transition for the nanocrystalline sample is shifted to the lower temperaturein comparison with the bulk for the smallest particle sized nanocrystalline sample (∼40nm). A large hysteresis is achieved in the temperature dependence <strong>of</strong> resistivity and the magneticfield dependence <strong>of</strong> magnetoresistance. Small magnetic field is required to melt the COfraction present in low temperature and large (∼100 %) low field magnetorestance hasbeen achieved at liquid nitrogen temperature.Anis Biswas, Indranil DasECMP4.1.1.12 Negligible domain wall contribution in magnetocaloric effect <strong>of</strong> GdPt 2Single-phase polycrystalline sample was prepared by argon arc melting. Specific heat measurementsboth in absence and in presence <strong>of</strong> magnetic field were performed using home made set-up.Magnetocaloric parameters ∆T ad and -∆S were obtained from the specific heat data.Fig.4.1.1.12. Low field magnetoresistance at the inset indicates significant domain wallcontribution in magnetoresistance. The hump in -∆ρ data around 10 K vanishes aftersubtracting domain wall contribution and the dependence becomes similar to -∆S-domain wall contribution in magneto caloric effect is insignificantMagnetoresistance measurements as a function <strong>of</strong> magnetic field as well as a function <strong>of</strong> temperaturewere carried out. There is qualitative difference between the temperature dependence <strong>of</strong> -∆ρ(=ρ(H)-ρ(0)) and -∆S. However after removing the domain wall scattering contribution from -∆ρ,the nature <strong>of</strong> -∆ρ and -∆S as a function <strong>of</strong> temperature is similar. Our study indicates thatthe domain wall contribution in MCE is negligibly small in spite <strong>of</strong> large contribution

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