Syntheses, structure, magnetism, and optical properties of the interlanthanide sulfides {delta}-Ln {sub 2-} {sub x} Lu {sub x} S{sub 3} (Ln=Ce, Pr, Nd)
- Department of Chemistry and Biochemistry and the E.C. Leach Nuclear Science Center, Auburn University, Auburn, AL 36849 (United States)
- Department of Physics and National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL 32310 (United States)
- Department of Physics and Astronomy, Tufts University, Medford, MA 02155 (United States)
- Chemical Sciences Division-Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720 (United States)
{delta}-Ln {sub 2-} {sub x} Lu {sub x} S{sub 3} (Ln=Ce, Pr, Nd; x=0.67-0.71) compounds have been synthesized through the reaction of elemental rare-earth metals and S using a Sb{sub 2}S{sub 3} flux at 1000 deg. C. These compounds are isotypic with CeTmS{sub 3}, which has a complex three-dimensional structure. It includes four larger Ln{sup 3+} sites in eight- and nine-coordinate environments, two disordered seven-coordinate Ln{sup 3+}/Lu{sup 3+} positions, and two six-coordinate Lu{sup 3+} ions. The structure is constructed from one-dimensional chains of LnS {sub n} (n=6-9) polyhedra that extend along the b-axis. These polyhedra share faces or edges with two neighbors within the chains, while in the [ac] plane they share edges and corners with other chains. Least square refinements gave rise to the formulas of {delta}-Ce{sub 1.30}Lu{sub 0.70}S{sub 3}, {delta}-Pr{sub 1.29}Lu{sub 0.71}S{sub 3} and {delta}-Nd{sub 1.33}Lu{sub 0.67}S{sub 3}, which are consistent with the EDX analysis and magnetic susceptibility data. {delta}-Ln {sub 2-} {sub x} Lu {sub x} S{sub 3} (Ln=Ce, Pr, Nd; x=0.67-0.71) show no evidence of magnetic ordering down to 5 K. Optical properties measurements show that the band gaps for {delta}-Ce{sub 1.30}Lu{sub 0.70}S{sub 3}, {delta}-Pr{sub 1.29}Lu{sub 0.71}S{sub 3}, and {delta}-Nd{sub 1.33}Lu{sub 0.67}S{sub 3} are 1.25, 1.38, and 1.50 eV, respectively. Crystallographic data: {delta}-Ce{sub 1.30}Lu{sub 0.70}S{sub 3}, monoclinic, space group P2{sub 1} /m, a=11.0186(7), b=3.9796(3), c=21.6562(15) A, {beta}=101.6860(10), V=929.93(11), Z=8; {delta}-Pr{sub 1.29}Lu{sub 0.71}S{sub 3}, monoclinic, space group P2{sub 1} /m, a=10.9623(10), b=3.9497(4), c=21.5165(19) A, {beta}=101.579(2), V=912.66(15), Z=8; {delta}-Nd{sub 1.33}Lu{sub 0.67}S{sub 3}, monoclinic, space group P2{sub 1} /m, a=10.9553(7), b=3.9419(3), c=21.4920(15) A, {beta}=101.5080(10), V=909.47(11), Z=8. - Graphical abstract: Inverse molar neodymium magnetic susceptibility vs. T for {delta}-Nd{sub 1.33}Lu{sub 0.67}S{sub 3} under an applied magnetic field of 0.1T between 2 and 300 K. The straight line represents the fit to Curie-Weiss law in the range of 100-300 K.
- OSTI ID:
- 21015883
- Journal Information:
- Journal of Solid State Chemistry, Vol. 180, Issue 7; Other Information: DOI: 10.1016/j.jssc.2007.04.008; PII: S0022-4596(07)00152-1; Copyright (c) 2007 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved; Country of input: International Atomic Energy Agency (IAEA); ISSN 0022-4596
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
ORGANIC
PHYSICAL AND ANALYTICAL CHEMISTRY
ANTIMONY SULFIDES
CERIUM COMPOUNDS
CRYSTALLOGRAPHY
CURIE-WEISS LAW
EV RANGE 01-10
LANTHANUM COMPOUNDS
LUTETIUM COMPOUNDS
LUTETIUM IONS
MAGNETIC FIELDS
MAGNETIC SUSCEPTIBILITY
MAGNETISM
MAGNETIZATION
MONOCLINIC LATTICES
NEODYMIUM COMPOUNDS
OPTICAL PROPERTIES
PRASEODYMIUM COMPOUNDS
SPACE GROUPS
SYNTHESIS
TEMPERATURE RANGE 0065-0273 K
TEMPERATURE RANGE 0273-0400 K