Structure and dynamics of superconducting NaxCoO2 hydrate and its unhydrated analog -: art. no. 214516

被引:103
作者
Lynn, JW [1 ]
Huang, Q
Brown, CM
Miller, VL
Foo, ML
Schaak, RE
Jones, CY
Mackey, EA
Cava, RJ
机构
[1] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[2] Univ Maryland, Dept Mat Engn, College Pk, MD 20742 USA
[3] Princeton Univ, Dept Chem, Princeton, NJ 08544 USA
[4] NIST, Div Analyt Chem, Gaithersburg, MD 20899 USA
[5] Princeton Univ, Princeton Mat Inst, Princeton, NJ 08544 USA
关键词
D O I
10.1103/PhysRevB.68.214516
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Neutron scattering has been used to investigate the crystal structure and lattice dynamics of superconducting Na0.3CoO2.1.4(H/D)(2)O, and the "parent" Na0.3CoO2 material. The structure of Na0.3CoO2 consists of alternate layers of CoO2 and Na and is the same as the structure at higher Na concentrations. For the superconductor, the water forms two additional layers between the Na and CoO2, increasing the c-axis lattice parameter of the hexagonal P6(3)/mmc space group from 11.16 Angstrom to 19.5 Angstrom. The Na ions are found to occupy a different configuration from the parent compound, while the water forms a structure that replicates the structure of ice. Both types of sites are only partially occupied. The CoO2 layer in these structures is robust, on the other hand, and we find a strong inverse correlation between the CoO2 layer thickness and the superconducting transition temperature (T-C increases with decreasing thickness). The phonon density of states for Na0.3CoO2 exhibits distinct acoustic and optic bands, with a high-energy cutoff of similar to100 meV. The lattice dynamical scattering for the superconductor is dominated by the hydrogen modes, with librational and bending modes that are quite similar to ice, supporting the structural model that the water intercalates and forms ice-like layers in the superconductor.
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相关论文
共 32 条
[1]   THE RESONATING VALENCE BOND STATE IN LA2CUO4 AND SUPERCONDUCTIVITY [J].
ANDERSON, PW .
SCIENCE, 1987, 235 (4793) :1196-1198
[2]   Refinement of the structure of Na0.74CoO2 using neutron powder diffraction [J].
Balsys, RJ ;
Davis, RL .
SOLID STATE IONICS, 1997, 93 (3-4) :279-282
[3]   Electronic model for CoO2 layer based systems:: Chiral resonating valence bond metal and superconductivity -: art. no. 097003 [J].
Baskaran, G .
PHYSICAL REVIEW LETTERS, 2003, 91 (09)
[4]   Superconductivity in a layered cobalt oxyhydrate Na0.31CoO2•1.3H2O [J].
Cao, GH ;
Feng, CM ;
Xu, Y ;
Lu, W ;
Shen, JQ ;
Fang, MH ;
Xu, ZA .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2003, 15 (33) :L519-L525
[5]  
CHOU FC, CONDMAT0306659
[6]   Chemical instability of the cobalt oxyhydrate superconductor under ambient conditions [J].
Foo, ML ;
Schaak, RE ;
Miller, VL ;
Klimczuk, T ;
Rogado, NS ;
Wang, Y ;
Lau, GC ;
Craley, C ;
Zandbergen, HW ;
Ong, NP ;
Cava, RJ .
SOLID STATE COMMUNICATIONS, 2003, 127 (01) :33-37
[7]   Observation of bulk superconductivity in NaxCoO2•yH2O and NaxCoO2•yD2O powder and single crystals -: art. no. 217001 [J].
Jin, R ;
Sales, BC ;
Khalifah, P ;
Mandrus, D .
PHYSICAL REVIEW LETTERS, 2003, 91 (21)
[8]   59Co NQR study on superconducting NaxCoO2•yH2O [J].
Kobayashi, Y ;
Yokoi, M ;
Sato, M .
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 2003, 72 (09) :2161-2164
[9]  
KUMAR B, CONDMAT0304210
[10]  
LARSON C, 1990, LAUR086748