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Specific Heat, Optical, and Transport Properties of Hexagonal Tungsten Bronzes

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Low Temperature Physics-LT 13

Abstract

The tungsten bronzes are a series of nonstoichimetric compounds of the general formula M x WO3, where M is usually an alkali metal atom. In this paper the cubic and hexagonal crystal structures are compared. Each structure is composed of linked WO6 octahedra, with M atoms filling the available cavities. In the cubic structure the WO6 matrix has rectangular channels in which the M atom is located. The cubic structure has all M sites full when x = 1. The hexagonal structure is composed of three- and six-member rings of WO6 octahedra. The M-atom sites are located in the hexagonal channels, with x = 1/3 corresponding to all sites full. The radii of the inscribed spheres of the cavities available for occupation by the M atoms are 0.96 Å and 2 Å in the cubic and hexagonal structures, respectively. The smaller M ions such as Na+ (0.95 Å) adopt the cubic structure for 0.5 ≲ x ≲ 1, whereas K+ (1.33 Å) and Rb+ (1.47 Å) form hexagonal bronzes.

Research supported by U.S. Air Force Office of Scientific Research, Office of Aerospace Research, under Grant No. AFOSR 68-1510C.

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© 1974 Springer Science+Business Media New York

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King, C.N., Benda, J.A., Greene, R.L., Geballe, T.H. (1974). Specific Heat, Optical, and Transport Properties of Hexagonal Tungsten Bronzes. In: Timmerhaus, K.D., O’Sullivan, W.J., Hammel, E.F. (eds) Low Temperature Physics-LT 13. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-2688-5_83

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  • DOI: https://doi.org/10.1007/978-1-4684-2688-5_83

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4684-2690-8

  • Online ISBN: 978-1-4684-2688-5

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