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I. Nowik Y. Levi I. Felner E. R. Bauminger C. Mermelstein 《Journal of Radioanalytical and Nuclear Chemistry》1995,190(2):413-418
Mössbauer studies of dilute57Fe and151Eu in RMn2Si2-xGex (R=La, Sm, Eu and Gd) at temperatures 4.2 K to 480 K have been performed. The diamagnetic iron and europium reveal the magnetic order of the Mn and rare earth sublattices through transferred hyperfine interactions. The57Fe studies show that in LaMn2Si2, LaMn2Ge2, and SmMn2Ge2 the Mn is magnetically ordered above the known Curie temperatures, and the compounds are antiferromagnets up to TN=470 K, 415 K and 385 K respectively. Studies of151Eu in R1-xEuxMn2Si2, (R=La, Gd) display Eu subspectra corresponding to Eu2+, Eu3+ and intermediate valant Eu. All display large magnetic hyperfine fields. 相似文献
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B. I. Belevtsev V. B. Krasovitsky D. G. Naugle K. D. D. Rathnayaka Glenn Agnolet I. Felner 《Bulletin of the Russian Academy of Sciences: Physics》2010,74(8):1049-1052
Magnetic and superconducting properties of polycrystalline samples of RuSr2Gd1.5Ce0.5Cu2O(10 − δ), asprepared (by solid-state reaction) and annealed in pure oxygen at different pressure are presented. Specific heat and
magnetization were investigated in the temperature range 1.8–300 K with a magnetic field up to 8 T. Specific heat, C (T), shows a jump at the superconducting transition (with onset at T ≈ 37.5 K) and a Schottky-type anomaly below 20 K. It is found that curves C(T) taken for different values of magnetic field have the same crossing point (at T
* ≈ 2.7 K) for all samples studied. At the same time, C(H) curves taken for different temperatures have a crossing point at a characteristic field H
* ≈ 3.7 T. These effects are manifestations of the crossing-point phenomenon, which is supposed to be inherent for strongly
correlated electron systems. 相似文献
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In order to check whether superconductivity occurs in the acceptor doped fullerenes C60(MF6)2 (M=As, P, Sb) and to study their magnetic and structural properties, we have carried out magnetic, EPR and NMR measurements of these compounds. Temperature dependences of magnetic susceptibility down to 5 K and field dependences of magnetic moment at 5 K show no ‘bulk’ transition in superconducting state. Some reasons of the absence of superconductivity, such as insufficient charge transfer between C60 and intercalated species and inhomogeneity of the compounds under study, are discussed. 相似文献
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Stoichiometric powdered FeYb2S4 having a cubic (special) spinel structure was prepared. The structure was based on X-ray diffraction and Mössbauer spectroscopy. The space group is Fd3m (No. 227) and the lattice constant a0 = 10.828Å. All the iron is divalent but only ca. 80% fills the tetrahedral 8a site while ca. 20% fills the octahedral 16d site. The ytterbium is trivalent, most of it occupying the normal octahedral 16d spinel site, but ca. 16% occupies the normally empty octahedral 16c site, having been displaced by the iron. 相似文献
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Mössbauer spectroscopy studies of151 Eu in EuBa2Cu3O7, EuBa2Cu3O6, EuBa2Cu3O6S, EuBaKCu3O7, EuBa2Cu2.5Fe0.5O7, Eu0.5Pr0.5Ba2Cu3O7, Eu1.25Ba1.75Cu3O7 and EuCaBaCu3O7 at several temperatures have been performed. The major conclusions are; All substitutions affect the Eu quadrupole interaction (10–20%). Substitution of 0 by S increases the Eu quadrupole interaction by 15% and increases η from 0.3 to 0.8 which proves that S substitutes oxygen in the immediate neighbourhood of the rare earth ions. In EuCaBaCu3O7 the quadrupole interaction is larger by 80% than in EuBa2Cu3O7, proving that in this structure Eu occupies predominantly the Ba sites. 相似文献
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Mössbauer studies of the 21.6 keV transition of151Eu in cubic EuBe13 and Eu1/2La1/2Be13 in the temperature range 100 K to 600 K have been performed. The position of the absorption line in EuBe13 moves from 0.60 mm/s at 100 K to 0.04 mm/s at 575 K. In Eu1/2La1/2B13 the line moves from 0.50 mm/s at 100 K to –0.03 mm/s at 500 K. We conclude that Eu in EuxLa1–xB13 is in an intermediate valence state and we analyze the temperature dependence of the isomer shift in terms of an interconfigurational fluctuation model. The model contains temperature independent parameters Eexc, the interconfiguration excitation energy, Tf, the valence fluctuation temperature, and S3, the isomer shift of pure Eu3+ in EuBe13. Assuming S3–S2= 13 mm/s the analysis yields S3=0.70 mm/s, Tf=400 K and Eexc=3000 K for EuBe13, whereas Tf=460 K and Eexc=2750 K for Eu1/2La1/2B13. 相似文献