Synthesis, structure and electrical properties of a new tin vanadium selenide

Abstract The turbostratically disordered misfit layer compound (SnSe) 1.15 VSe 2 was synthesized and structurally characterized. Electrical transport measurements suggest this compound undergoes a charge or spin density wave (CDW or SDW) transition, which has not been observed in previous misfit layer compounds. The (SnSe) 1.15 VSe 2 compound, created through the modulated elemental reactants technique, contains highly oriented intergrowths of SnSe bilayers and VSe 2 structured Se–V–Se trilayers with abrupt interfaces between them perpendicular to the c -axis. X-ray diffraction data and transmission electron microscope images show that each constituent has in-plane crystallinity but that there is a random rotational disorder between the constituent layers. Temperature-dependent electrical resistivity data and Hall measurements are consistent with (SnSe) 1.15 VSe 2 being a metal, however an abrupt increase in the resistivity occurs between 30 and 100 K. The carrier concentration decreases by approximately 1 carrier per vanadium atom during this temperature interval.

[1]  J. Morales,et al.  Lithium intercalation into PbNb2S5, PbNbS3, SnNb2Se5, BiVS3, SnVSe3, and PbNb2Se5 misfit layer chalcogenides , 1992 .

[2]  S. Amelinckx,et al.  Misfit layer compounds (MS)nTS2 (M = Sn, Pb, Bi, rare earth elements: T = Nb, Ta ; n = 1.08 – 1.19), a new class of layer compounds , 1989 .

[3]  HernanLourdes,et al.  Preparation and Characterization of New Misfit Layer Selenides SnVSe3 and SnNb2 Se5 , 1991 .

[4]  A. Meerschaut,et al.  CHALCOGENIDE MISFIT LAYER COMPOUNDS , 1995 .

[5]  David C. Johnson,et al.  Rational Synthesis and Characterization of a New Family of Low Thermal Conductivity Misfit Layer Compounds [(PbSe)0.99]m(WSe2)n† , 2010 .

[6]  S. Smaalen,et al.  THE INCOMMENSURATE MISFIT LAYER STRUCTURE OF (PBS)1.14NBS2, PBNBS3 AND (LAS)1.14NBS2, LANBS3 - AN X-RAY-DIFFRACTION STUDY , 1990 .

[7]  D. Cahill,et al.  Low thermal conductivity in nanoscale layered materials synthesized by the method of modulated elemental reactants , 2008 .

[8]  David Michael Rowe,et al.  Modules, Systems, and Applications in Thermoelectrics , 2012 .

[9]  M. J. Sienko,et al.  Anomalous electrical and magnetic properties of vanadium diselenide , 1976 .

[10]  J. Wilson,et al.  Charge-Density Waves in Metallic, Layered, Transition-Metal Dichalcogenides , 1974 .

[11]  A. H. Thompson,et al.  Correlated magnetic and transport properties in the charge-density-wave states of VSe2 , 1979 .

[12]  D. Eaglesham,et al.  Charge-density-wave transitions in 1T-VSe2 , 1986 .

[13]  Sander van Smaalen,et al.  Incommensurate crystal structures , 1995 .

[14]  K. Rossnagel On the origin of charge-density waves in select layered transition-metal dichalcogenides , 2011, Journal of physics. Condensed matter : an Institute of Physics journal.

[15]  A. Herzing,et al.  Synthesis and Electronic Properties of the Misfit Layer Compound [(PbSe)1.00]1[MoSe2]1 , 2010 .

[16]  S. Smaalen,et al.  X-RAY CRYSTAL-STRUCTURE DETERMINATION OF THE TRICLINIC MISFIT LAYER COMPOUND (SNS)1.20TIS2 , 1991 .

[17]  G. Wiegers Misfit layer compounds : Structures and physical properties , 1996 .

[18]  K. Koumoto,et al.  Low-Thermal-Conductivity (MS)1+x(TiS2)2 (M = Pb, Bi, Sn) Misfit Layer Compounds for Bulk Thermoelectric Materials , 2010, Materials.

[19]  W. Y. Zhou,et al.  THE MISFIT LAYER COMPOUND (SNSE)1.16NBSE2 , 1991 .

[20]  A. Meerschaut,et al.  Preparation, structure determination and transport properties of a new misfit layer compound : (PbS)1.14(NbS2)2 , 1990 .

[21]  A. Stacy,et al.  Effect of nonstoichiometry on the periodic lattice distortion in vanadium diselenide , 1980 .

[22]  A. Briggs,et al.  Critical Magnetic Field Measurements of the Misfit Layer Compound (SnS)1.17(NbS2) down to 50mK , 1998 .

[23]  David C. Johnson,et al.  Synthesis of [(SnSe)1.15]m(TaSe2)n Ferecrystals: Structurally Tunable Metallic Compounds , 2012 .

[24]  K. Chopra,et al.  POLYMORPHISM IN SOME IV‐VI COMPOUNDS INDUCED BY HIGH PRESSURE AND THIN‐FILM EPITAXIAL GROWTH , 1967 .

[25]  C. F. V. Bruggen,et al.  MAGNETIC-SUSCEPTIBILITY AND ELECTRICAL-PROPERTIES OF VSE2 SINGLE-CRYSTALS , 1976 .

[27]  A. Briggs,et al.  Superconductivity in the misfit layer compounds (BiSe)1.10(NbSe2) and (BiS)1.11(NbS2) , 1997 .

[28]  E. Krasovskii,et al.  Charge transfer in misfit layered compounds , 2003 .

[29]  David C. Johnson,et al.  Deposition system for the synthesis of modulated, ultrathin‐film composites , 1993 .

[30]  J. Baas,et al.  Vacancies and electron localization in the incommensurate intergrowth compound (La0.95Se)1.21VSe2 , 1996 .

[31]  J. Wilson,et al.  Effects of doping on charge-density waves in layer compounds , 1975 .

[32]  A. Williams,et al.  Superconductivity at 2.3 K in the misfit compound (PbSe) 1.16(TiSe2)2 , 2010, 1006.5946.

[33]  David C. Johnson,et al.  Determination of the composition of Ultra-thin Ni-Si films on Si: constrained modeling of electron probe microanalysis and x-ray reflectivity data , 2008 .

[34]  David C. Johnson,et al.  The synthesis and characterization of new [(BiSe)1.10]m[NbSe2]n, [(PbSe)1.10]m[NbSe2]n, [(CeSe)1.14]m[NbSe2]n and [(PbSe)1.12]m[TaSe2]n misfit layered compounds ☆ , 2008 .

[35]  E. Makovicky,et al.  Incommensurate, Two-Layer Structures with Complex Crystal Chemistry: Minerals and Related Synthetics , 1992 .