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Evolution of Bonding and Magnetism via Changes in Valence Electron Count in CuFe2-xCoxGe2.
Tener, Zachary P; Yannello, Vincent; Garlea, V Ovidiu; Lapidus, Saul H; Yox, Philip; Kovnir, Kirill; Stoian, Sebastian A; Shatruk, Michael.
Afiliação
  • Tener ZP; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, United States.
  • Yannello V; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, United States.
  • Garlea VO; Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United States.
  • Lapidus SH; X-ray Science Division, Argonne National Laboratory, Argonne, Lemont, Illinois 60439, United States.
  • Yox P; Department of Chemistry, Iowa State University, Ames, Iowa 50011, United States.
  • Kovnir K; Ames Laboratory, United States Department of Energy, Ames, Iowa 50011, United States.
  • Stoian SA; Department of Chemistry, Iowa State University, Ames, Iowa 50011, United States.
  • Shatruk M; Ames Laboratory, United States Department of Energy, Ames, Iowa 50011, United States.
Inorg Chem ; 61(10): 4257-4269, 2022 Mar 14.
Article em En | MEDLINE | ID: mdl-35225605
ABSTRACT
A series of solid solutions, CuFe2-xCoxGe2 (x = 0, 0.2, 0.4, 0.8, and 1.0), have been synthesized by arc-melting and characterized by powder X-ray and neutron diffraction, magnetic measurements, Mössbauer spectroscopy, and electronic band structure calculations. All compounds crystallize in the CuFe2Ge2 structure type, which can be considered as a three-dimensional framework built of fused MGe6 octahedra and MGe5 trigonal bipyramids (M = Fe and Co), with channels filled by rows of Cu atoms. As the Co content (x) increases, the unit cell volume decreases in an anisotropic fashion the b and c lattice parameters decrease while the a parameter increases. The changes in all the parameters are nearly linear, thus following Vegard's law. CuFe2Ge2 exhibits two successive antiferromagnetic (AFM) orderings, corresponding to the formation of a commensurate AFM structure, followed by an incommensurate AFM structure observed at lower temperatures. As the Co content increases, the AFM ordering temperature (TN) gradually decreases, and only one AFM transition is observed for x ≥ 0.2. The magnetic behavior of unsubstituted CuFe2Ge2 was found to be sensitive to the preparation method. The temperature-dependent zero-field 57Fe Mössbauer spectra reveal two hyperfine split components that evolve in agreement with the two consecutive AFM orderings observed in magnetic measurements. In contrast, the field-dependent spectra obtained for fields ≥2 T reveal a parallel arrangement of the moments associated with the two crystallographically unique metal sites. Electronic band structure calculations and chemical bonding analysis reveal a mix of strong M-M antibonding and non-bonding states at the Fermi level, in support of the overall AFM ordering observed in zero field. The substitution of Co for Fe reduces the population of the M-M antibonding states and the overall density of states at the Fermi level, thus suppressing the TN value.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article