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Biennial Report 2005-2007 - Saha Institute of Nuclear Physics

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112 <strong>Biennial</strong> <strong>Report</strong> <strong>2005</strong>-07being developed for the data collection by the computer. The work is in progress.S Das, A Pal, A Chakrabarty, BG GhoshECMP4.1.1.18 Anomalous transport properties <strong>of</strong> Co-site impurity doped Na x CoO 2The effect <strong>of</strong> substitution <strong>of</strong> Cu, Zn, Ga, Mn and Ni for Co on resistivity (ρ), magnetization (M)and thermopower (S) in layered Na x CoO 2 has been investigated. At low temperature, ρ remainsmetallic (dρ/dT >0) for Cu, Zn and Ga impurities over the entire range <strong>of</strong> doping while for Mnand Ni a metal-insulator transition occurs at or above 3 percent doping. For Cu-doped samples,ρ(T) shows strong anomaly and hysteresis at around 280 K where a first-order structural phasetransition occurs due to the long-range ordering <strong>of</strong> Na-vacancy clusters. The magnetic susceptibilityexhibits Curie-Weiss law. The Neel temperature is insensitive to impurity while Curie constant andWeiss constant (θ) depend both on the nature and amount <strong>of</strong> impurity. A small enhancement <strong>of</strong>magnetization above 280 K and the increase <strong>of</strong> θ with Cu doping are the signatures <strong>of</strong> Na-vacancyordering. In contrast to ρ and M, S changes systematically with doping and temperature, anddoes not show anomalous behavior around 280 K.Prabhat MandalECMP4.1.1.19 Transport properties <strong>of</strong> doped RuSr 2 GdCu 2 O 8 superconductorThe transport properties <strong>of</strong> Ru 1−x M x Sr 2 GdCu 2 O 8 (Ru-1212), with M = Ti, Rh and Sn for 0 ≤x ≤ 0.2, have been studied. Both thermoelectric power (S) and resistivity (ρ) measurementsare discussed and compared with those <strong>of</strong> Ru(Sr 1−x L x )GdCu 2 O 8 , where L is La and Na, with0 ≤ x ≤ 0.10. The superconducting and normal state properties <strong>of</strong> Ru-1212 depend strongly on thetype <strong>of</strong> dopant and the substitutional site. It is noticed that T c is reduced for all doped compoundseven for Ti, Rh and Na doping where a small decrease in S is observed. The behavior <strong>of</strong> both S(T)and ρ(T) indicates that Ru-1212 superconductor is similar to other underdoped cuprate systems.A Hassen, Prabhat MandalECMP4.1.1.20 Volume contraction and resistivity drop at the Jahn-Teller transition inLa 1−x Ca x MnO 3We have investigated the Jahn-Teller transition accompanied by orbital order-disorder transitionin La 1−x Ca x MnO 3 by high temperature X-ray powder diffraction with synchrotron radiation andresistivity measurements. The unit cell volume <strong>of</strong> LaMnO 3 decreases with increasing temperaturein a narrow temperature range below T JT =750 K and then undergoes a volume collapse at T JT .The transition is first order. Similar behavior is also obtained in Ca-doped La 1−x Ca x MnO 3 forx=0.025 and 0.075. The amount <strong>of</strong> volume collapse, however, decreases with the doping and alsothe first order discontinuous transition crosses over to a quasi-continuous transition with doping.We interpret the volume contraction at the transition is due to a more efficient packing <strong>of</strong> theMnO 6 octahedra in the orbitally liquid state and the crossover from the discontinuous to the

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