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23 April 2024
 
  » arxiv » cond-mat/0412122

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Resistivity and Thermoelectric power of NaxCoO2 (x =1.0, 0.7 and 0.6) system
H. Kishan ; V.P.S. Awana ; M.A. Ansari ; Anurag Gupta ; R.B. Saxena ; V. Ganesan ; A.V. Narlikar ; C. A. Cardoso ; R. Nirmala ; Devendra Buddhikot ; S.K. Malik ;
Date 6 Dec 2004
Subject Strongly Correlated Electrons; Superconductivity | cond-mat.str-el cond-mat.supr-con
AffiliationNPL, New Delhi, India) V. Ganesan and A.V. Narlikar (IUC, Indore, INDIA), C. A. Cardoso (Univ. Maryland USA), R. Nirmala, Devendra Buddhikot and S.K. Malik (TIFR, Mumbai, India
AbstractResults of thermo-electric power (S) and electrical resistivity (r) measurements are reported on NaxCoO2 compounds with x = 1.0, 0.7 and 0.6. These are single-phase compounds crystallizing in the hexagonal structure (space group P63/mmc) at room temperature. Thermo-electric power values at 300K (S300K) are, 80mV/K, 39mV/K and 37mV/K for x = 1.0, 0.7 and 0.6 samples, respectively. The samples with x=0.7 and 1.0 are metallic down to 5 K, while the x = 0.6 sample is semiconducting. The value of r300K for x = 1.0 sample is ~0.895 mW-cm and the power factor (S2/r) is = 7.04 x 10-3 W/mK2 which qualifies it as a good thermo-electric material. In x =1.0 sample, S(T) is positive throughout 300-5K temperature range and decreases monotonically to zero as temperature T= 0. In contrast, S(T) of x = 0.7 and 0.6 samples changes sign and shows negative values between 90 K and 16 K before approaching zero as T = 0. Anomalous S(T) behavior of x = 0.6 and 0.7 samples, which are coincidentally the precursor materials to the reported superconductivity in this class of materials, indicates a dramatic change in the electronic structure of these compounds on lowering the Na content.
Source arXiv, cond-mat/0412122
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