Download Actinide Monochalcogenides: Pnictides and Chalcogenides III by R. Troć (auth.), H.P.J. Wijn (eds.) PDF

By R. Troć (auth.), H.P.J. Wijn (eds.)

The Landolt-Börnstein quantity 27 offers with the magnetic homes of non-metallic inorganic compounds in keeping with transition parts, akin to there are pnictides, chalcogenides, oxides, halides, borates, silicates and phosphates. A survey of the contents of all subvolumes that experience already seemed or were deliberate to seem is outlined at the within front disguise. so one can conceal the massive volume of magnetic and magnetically comparable homes of the lanthanide and actinide pnictides and chalcogenides that seemed in literature lately, the subvolume 27B needed to be break up into subvolumes B1...B8. Subvolumes 27B1, 27B2, 27B3, 27B4 and 27B5 (published among 1998 and 2003) care for lanthanide pnictides and chalcogenides. Pnictides are outlined as compounds containing at the least one of many components P, As, Sb or Bi (V-th team of the Periodic System), and chalcogenides are outlined as compounds containing one of many parts S, Se or Te (VI-th staff of the periodic system). the 3 subvolumes 27B6, 27B7 and 27B8 hide the houses of actinide pnictides and chalcogenides. Subvolume 27B8 (published in 2004) offers with ternary actinide pnictides and chalcogenides, whereas in subvolume 27B7 (published in 2005) information on binary non-equiatomic actinide pnictides and chalcogenides are given.

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30 (2004) 305. : Physica B 345 (2004) 221. : J. Alloys Compd. 366 (2004) 15-20. : Physica B 378-380 (2006) 976. : J. Alloys Compd. 414 (2006) 14. : J. Magn. Magn. Mat. 310 (2007) 1781. : J. Phys. Cond. Mater. 19 (2007) 236204. 1007/978-3-540-47043-4_3 ß Springer 2009 Landolt‐Bo¨rnstein New Series III/27B6β Survey: Actinide Monosulfides (AnS) 4 Survey: Actinide Monosulfides (AnS) Unless stated otherwise,  An stands for actinides U, Np, Pu;  X stands for pnicogens P, As, Sb;  Y stands for chalcogens S, Se, Te.

Cation/anion radius ratio, rC/rA Phase transition pressure, pt, vs. 10a Volume change, ΔV/V0, vs. 10b ThY (ThX) UY (UX) Lattice parameter, a0(AnY), vs. lattice parameter, a0(GdY), and a0(AnX) vs. 18 Photoemission spectral 5f, 6d line width (FWHM), Γ, vs. U-U distance, dU-U Inset Photoemission spectral 5f, 6d line width (FWHM), Γ, vs. 21a 79REG Electron spin polarization vs. 21b UY (UX) Experimental lattice parameter, a0, vs. 24 (aThY(X)−aUY(X)), vs. U-U distance, dU-U UY Cubic rhombohedral distortion of the fcc unit cell and corresponding interaxial angles, pffiffiffi αC or αR, ΔαR=2/ 3 ΔαC Landolt‐Bo¨rnstein New Series III/27B6β 87R 82RMV Molar volume, V0, vs.

Appl. Phys. 53 (1982) 2008. : High Pressure Measurements Techniques, Allied Science, New York, 1983 p. 133. : J. Less-Comm. Met. 100 (1984) 153. : J. Phys. F, Met. Phys. 14 (1984) 639. : J. Less-Comm. Met. 98 (1984) 301. J. H. ), Amsterdam: North Holland, 1984, Vol. 1, pp. 1-77. : J. Solid State Com. 52 (1984) 203. , in: 17th Int. Conf. , 1984, pp. 167-168. : J. Appl. Phys. 55 (1984) 1853. J. and Lander, G. H. ), Amsterdam: North Holland, 1984, Vol. 1, pp. 341-414. : Phys. Rev. B 30 (1984) 6578.

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