Resolving Composition and Structure of RE–Sb–O–C Natural Superlattice Phases (RE = La, Ho)

A family of rare earth antimonide oxycarbides have been prepared and structurally characterized. These superlattice phases are constructed from NaCl-type RESb slabs sandwiched between RE–O–C layers. Depending on the carbon content and synthetic conditions, three different RE–Sb–O–C structures can be obtained. At lower temperatures,RE9–δSb5(O,C)5 phases are obtained for RE = La, Ho. These phases adopt a stuffed Sc2Sb-type structure with P4/nmm symmetry. An O/C mixture, in which the O/C ratio is larger than 4:1, is randomly distributed within the RE–O–C layers. The RE atoms are highly disordered within the oxide layer. At temperatures above the melting point of the samples, RE9Sb5O4C phases with P4/n symmetry are produced. The RE–O–C layers in RE9Sb5O4 are fully ordered; the RE sites are well defined, and the O and C atoms occupy the tetrahedral and square-pyramidal voids, respectively. At high temperatures, a new ordered La14Sb8O7C structure with P4bm symmetry was discovered. The La14Sb8O7C phase is structurally similar to RE9Sb5O4C and features orderedarrangements of La and O/C atoms in the La–O–C layer. The RE9–δSb5(O,C)5, RE9Sb5O4C and La14Sb8O7C phases appear to be charge-balanced, and their compositions and structures are controlled by the O/C ratio. Parallel preparative experiments revealed the importance of carbon in the formation of these layered phases. In addition, it has been established that the purity of the rare earth metals influences the compositions and structures of the products.

[1]  S. Forbes,et al.  Synthesis, crystal and electronic structures of new narrow-band-gap semiconducting antimonide oxides RE(3)SbO(3) and RE(8)Sb(3-delta)O(8), with RE = La, Sm, Gd, and Ho. , 2010, Journal of the American Chemical Society.

[2]  M. Jansen,et al.  Crystal Structure Of Terbium Antimonide Oxide, Tb9Sb9O5 , 2009 .

[3]  G. J. Snyder,et al.  Complex thermoelectric materials. , 2008, Nature materials.

[4]  G. Sheldrick A short history of SHELX. , 2008, Acta crystallographica. Section A, Foundations of crystallography.

[5]  M. Jansen,et al.  Reticular merohedral twinning within the La9Sb5O5 structure family: structure of Pr9Sb5O5, Sm9Sb5O5 and Dy9Sb5O5. , 2007, Acta crystallographica. Section B, Structural science.

[6]  J. Corbett,et al.  Hydrogen in Polar Intermetallics. Binary Pnictides of Divalent Metals with Mn5Si3-type Structures and Their Isotypic Ternary Hydride Solutions , 2006 .

[7]  K. Koumoto,et al.  Complex Oxide Materials for Potential Thermoelectric Applications , 2006 .

[8]  Sossina M. Haile,et al.  Zintl Phases as Thermoelectric Materials: Tuned Transport Properties of the Compounds CaxYb1–xZn2Sb2 , 2005 .

[9]  Z. Kang,et al.  Binary rare earth oxides , 2005 .

[10]  H. Schnering,et al.  Über die Antimonidoxide La9Sb5O5 und Ce9Sb5O5 sowie die binären Phasen La2Sb und Ce2Sb , 2004 .

[11]  Daniel Vivien,et al.  A simple model for the prediction of thermal conductivity in pure and doped insulating crystals , 2003 .

[12]  F. Disalvo,et al.  Thermoelectric cooling and power generation , 1999, Science.

[13]  K. Gschneidner,et al.  MAGNETIC PHASE TRANSITIONS AND THE MAGNETOTHERMAL PROPERTIES OF GADOLINIUM , 1998 .

[14]  Kwon,et al.  Electrical transport properties of semimetallic GdX single crystals (X=P, As, Sb, and Bi). , 1996, Physical review. B, Condensed matter.

[15]  K. Gschneidner,et al.  Solid state electrotransport purification of dysprosium , 1995 .

[16]  D. W. Jones,et al.  Tetragonal and cubic crystal structures of some binary and ternary metal dicarbides in the series Ce-Er, Ce-Lu, U-La, and U-Ce , 1991 .

[17]  Michael O'Keeffe,et al.  Bond-valence parameters for solids , 1991 .

[18]  D. W. Jones,et al.  A neutron-diffraction study of the tetragonal crystal structures of some yttrium-holmium dicarbides , 1984 .