1992
DOI: 10.1103/physrevb.46.9341
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Neutron-scattering studies on CeM2Ge2(M=Ag, Au, and Ru)

Abstract: The results of elastic, quasielastic, and inelastic neutron-scattering studies on polycrystalline CeM2Ge2 (M=Ag, Au, and Ru) are presented. All compounds reveal long-range magnetic order at low temperatures. Ferromagnetic (M=Ru), antiferromagnetic (M=Au), and incommensurate (M=Ag) structures were detected. Using time-of-flight (TOF) techniques, the crystalline electric-field splittings were determined. With high-resolution TOF experiments the temperature and wave-vector dependence of the magnetic relaxation ra… Show more

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Cited by 76 publications
(65 citation statements)
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“…The magnetic susceptibility of CeAu 2 Ge 2 exhibits strong anisotropy with an easy [001] direction perpendicular to the tetragonal plane. 16,17 Previous measurements on a powder of CeAu 2 Ge 2 showed that the correlated Ce-ions develop a long range antiferromagnetic order below T N 16 K. 13 In this article, we report elastic neutron scattering measurements on a high quality single crystal sample of CeAu 2 Ge 2 . The crystals were synthesized by high temperature solution growth method using Bi flux and the quality was verified using X-ray measurements.…”
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confidence: 99%
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“…The magnetic susceptibility of CeAu 2 Ge 2 exhibits strong anisotropy with an easy [001] direction perpendicular to the tetragonal plane. 16,17 Previous measurements on a powder of CeAu 2 Ge 2 showed that the correlated Ce-ions develop a long range antiferromagnetic order below T N 16 K. 13 In this article, we report elastic neutron scattering measurements on a high quality single crystal sample of CeAu 2 Ge 2 . The crystals were synthesized by high temperature solution growth method using Bi flux and the quality was verified using X-ray measurements.…”
mentioning
confidence: 99%
“…19,20 Previous as well as recent work on both polycrystalline and single crystal samples suggest that the crystal field level scheme in CeAu 2 Ge 2 consists of three doublets at ∆ 0 = 0 K, ∆ 1 12 meV and ∆ 2 18 meV. 13,16 The ground state is almost pure J z = ±5/2 with an admixture of ±3/2. The first excited doublet state is high enough in energy to avoid any significant intermixing between the ground and first excited state doublets, so that any induced moment magnetic state is highly unlikely.…”
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confidence: 99%
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