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1.
In a recent study of the magnetic order in Gd3Ag4Sn4 by neutron powder diffraction and 119Sn Mössbauer Spectroscopy we showed that both the Gd(2d) and Gd(4e) sublattices order antiferromagnetically at 28.8(2) K. We also demonstrated that the ‘magnetic event’ around 8 K is in fact a ‘plane to axis’ spin-reorientation of the Gd magnetic structure. Here, we extend our study with 155Gd Mössbauer Spectroscopy. The initial magnetic ordering at 30(2) K is clear for both sites and substantial changes in the hyperfine fields are observed at 8 K when the magnetic structure reorients.  相似文献   

2.
N Lakshmi  K Venugopalan  J Varma 《Pramana》2002,59(3):531-537
Heusler-like alloy Fe2CrAl was prepared and studied. Structure determination was done by X-ray. The structure was found to conform to the B2 type. Magnetic hyperfine fields in this sample were studied by the Mössbauer effect. The Mössbauer spectra were recorded over a range of temperature from 40 to 296 K. The Mössbauer spectra showed the co-existence of a paramagnetic part with a magnetic hyperfine portion at all recorded temperatures. Even with the distribution in the magnetic hyperfine field, the average hyperfine field follows the (T/T c)3/2 law. The paramagnetic part of the hyperfine field is explained in terms of the clustering of Cr atoms.  相似文献   

3.
The Mössbauer spectra of (Fe, Co)S1 + x were recorded at room temperature and 4.2 K for samples of varying composition to study the magnetic behaviour of the solid solutions. The Mössbauer spectra are split magnetically at iron concentrations above 16% Fe. For samples with less than 16%Fe, the Mössbauer spectra show no evidence of magnetic splitting down to 4.2 K. The room temperature centre shift data appear to vary continuously with composition and the hyperfine magnetic field decreases with decreasing Fe2+ concentration. A Mössbauer spectrum of 57Fe:CoS at 4.2 K in an external field of 25 kOe showed no evidence of magnetic splitting beyond that caused by the applied field, indicating a net zero internal field.A high spin to low spin transition in Fe2+ is ruled out as being responsible for the observed magnetic behaviour on the basis of the centre shift data. The Mössbauer data are interpreted to indicate a substantial increase in electron delocalization towards the ligands as the 〈M-S〉 distance decreases with decreasing Fe2+concentration. This causes a reduction in the magnitude of the internal magnetic field contributions as well as a decrease of shielding of the nucleus, giving rise to the observed Mössbauer parameters.The Mössbauer spectrum of 57Fe:CoS at room temperature is compared with the spectrum of FeS above the 6.7 GPa phase transition at room temperature. The similarities of the centre shift and the 〈M-S〉 distance in the two phases indicate that covalency may also be responsible for the observed high pressure behaviour of FeS, and not the presence of Fe3+ as was originally suggested.  相似文献   

4.
Mössbauer and magnetic measurements have been performed at various temperatures between 1.5K and 300K on a natural hedenbergite Ca0.96 Mg0.19 Fe0.82Mn0.02Si2O6. The magnetic measurements are consistent with a ferromagnetic alignment of the Fe2+ moments inside each zig-zag M1 chain and antiferromagnetic alignment of the moments of neighbouring chains. Above TN (Mössbauer)=29±2K, a single quadrupole doublet attributed to Fe2+ in the M1 sites is observed. At 4.2K, the Mössbauer spectra can be accounted for by a discrete distribution of six hyperfine field components which can be related to all the possible Fe2+?Mg2+ configurations up to second cation neighbours surrounding a central57Fe2+ probe.  相似文献   

5.
Montmorillonite particles were modified by iron oxides using the precipitation process with the aim to monitor the differences in the structural and magnetic properties of intercalated and adsorbed Fe3+. The Mössbauer spectra recorded at 5 K in zero and 6 T external fields, IR spectra and TG curves measured in zero and 32 mT fields identified the ferrihydrite pillars in an interlayer space of the montmorillonite structure and γ-Fe2O3 nanoparticles adsorbed on the mineral surface. The temperature dependent Mössbauer spectra (25–300 K) reflect the superparamagnetic behaviour of maghemite nanoparticles and ferrihydrite pillars with the blocking temperatures of about 80 and 25 K, respectively.  相似文献   

6.
Samples of the magnetism-zinc ferrite series ZnxMg1?xFe2O4 (x = 0.0 to 1.0) have been studied by the Mössbauer effect technique at 77 K. Mössbauer spectra for x = 0.0 to 0.6 suggest the existence of two hyperfine fields, one due to the Fe3+ tetrahedral ions (A-sites) and the other due to the Fe3+ octachedral ions (B-sites), while for x=0.7 it shows relaxation behaviour and for x?0.8 it exhibits a paramagnetic quadrupole doublet. The variation of nuclear magnetic fields at the A and B sites is explained on the basis of the AB and BB supertransferred hyperfine interactions. Analysis of the average Mössbauer line width as a function of zinc concentration suggests that the relaxation spectrum observed at x=0.7 (77 K) is possibly due to domain wall oscillations.  相似文献   

7.
Nasu  S.  Kawakami  T.  Kawasaki  S.  Takano  M. 《Hyperfine Interactions》2002,144(1-4):119-127

Using a diamond anvil cell and a low-temperature cryostat with a superconducting solenoid, high-pressure 57Fe Mössbauer spectroscopy with a radioactive source at 4.5 K under external magnetic fields up to 7 T has been developed. Pressure-temperature magnetic phase-diagrams for perovskite iron oxides, SrFeO3, CaFeO3 and Sr2LaFe3O9 are presented up to about 70 GPa. High-pressure Mössbauer measurements under external magnetic fields proved that the electronic ground states of these oxides switch to uniform-charge and ferromagnetic (and most probably metallic) states under extremely high pressure.

  相似文献   

8.
Polycrystalline Fe2BO4 was prepared by solid state reactions and its electronic and magnetic properties were investigated by Mössbauer spectroscopy and magnetization measurements. The Mössbauer spectra of Fe2BO4 below 270 K indicate the presence of Fe2+ and Fe3+ sites in the structure, in a ratio 1 : 1. Above this temperature electron delocalization sets in between the divalent and trivalent iron ions and Fe2.5+ states are observed. The temperature dependence of the Mössbauer spectra and magnetization measurements clearly show the onset of magnetic order below 155 K.  相似文献   

9.
Low temperature 57Fe Mössbauer spectra of mechanically alloyed EuFeO3 prepared by mechanical alloying depicts an interesting transformation in its hyperfine magnetic state, from a triple phase magnetic system at room temperature to a single phase ferromagnetic state at 20 K. The hyperfine magnetic field increased by 12% at 20 K from its room temperature. The isomer shift and quadrupole splitting values exhibit a peak around 200 K. Low temperature 151Eu Mössbauer measurements show that the line-width increased to its maximum value at 80 K which is 45% compared to its room temperature value not enough to suggest splitting.  相似文献   

10.
Magnetic properties of the FeTe0.8S0.2 superconductor were studied by Mössbauer spectroscopy. Low-velocity Mössbauer spectra that were recorded in the temperature range from 5.7 K up to 300 K show a paramagnetic doublet with a broadening at temperatures below 77 K. The broadening can be explained by the appearance of a distribution of hyperfine magnetic fields due to the magnetic ordering of a part of the sample. The magnetically ordered fraction starts to decrease at temperatures below 20 K indicating a possible competition with the onsetting superconductive state.  相似文献   

11.
57Fe and 237Np Mössbauer ōmeasurements have been performed for NpFeGa5, which is one of the so-called neptunium 1-1-5 compounds. The 57Fe Mössbauer spectra below T N = 118 K show the magnetically ordered state. The magnitude of the hyperfine magnetic field at the 57Fe nucleus is determined to be 1.98 ± 0.05 T at 10 K. From the 237Np Mössbauer spectrum at 10 K, the hyperfine magnetic field at the 237Np nucleus is 203 T and the hyperfine coupling constant is determined to be 237 T/μB using the Np atomic magnetic moment of 0.86 μB determined by the neutron diffraction study.  相似文献   

12.
Ultrafine amorphous FeNiB powder has been prepared by borohydride reduction by mixing the aqueous solutions. The influence of the mixing way and the drying procedure was observed. The paramagnetic doublet component of the Mössbauer spectra indicates the existense of the Fe3+, whose state was discussed. The Mössbauer measurements have been performed at room temperature (RT) and at 77K. The effect of the magnetic fields on the amorphous powders was somehow analogous to that on amorphous ribbons produced by a melt spinning method. The spontaneous magnetization of the flaky powder sample tended to locate on the sample plane.  相似文献   

13.
Mössbauer studies have been performed on FePS3 in powder form between 125 K and 450 K. The Mössbauer spectrum consists of an asymmetric doublet, ratio~0.93 at room temperature. The asymmetry is attributed to the Goldanskii-Karyagin effect and the lattice anisotropy is found to be ~1.4, with the largest vibrations parallel to thec ? axis of the monoclinic unit cell. The Debye temperature is ~200 K.  相似文献   

14.
Split source57Fe Mössbauer effect spectroscopy has been performed between 4 K and 295 K on the superconducting perovskite GdBa2Cu3O7?y. No evidence is seen for magnetic splitting at low temperatures as reported in some split absorder57Fe Mössbauer experiments on this material. There is evidence for phonon mode softening, as observed for119Sn Mössbauer spectra of some other highT c superconductors.  相似文献   

15.
A high transmission spherical electrostatic electron spectrometer for Mössbauer conversion electron spectroscopy was built. Depth selective Mössbauer studies can be carried out from T=4 K to 350 K in a 10?8 Torr vacuum changing the electron energies and/or the electron escape angles.  相似文献   

16.
The solid state solutions of europium transition element oxides Eu (Fe0.8M0.2)O3 (M=Sc,Cr,Mn,Co) are synthesized. The X-ray diffraction of the compound shows that all the compounds possess the perovskite structures. Both the151Eu Mössbauer spectra and the57Fe Mössbauer spectra are measured. The hyperfine magnetic field and non-axisymmetric electric field gradient are observed in the151Eu Mössbauer spectrum. The57Fe Mössbauer spectrum shows that there are four components of hyperfine fields corresponding to four kinds of different neighbours of the Fe ion.  相似文献   

17.
We present crystallographic and magnetic properties of NiCr1.98 57Fe0.02O4 by using X-ray diffractometry (XRD), vibrating sample magnetometry (VSM), and Mössbauer spectroscopy. The lattice constants a0 were determined to be 8.318 Å. The ferrimagnetic Neel temperature (T N) for NiCr1.98 57Fe0.02O4 is determined to be 90 K. The Mössbauer absorption spectra for all chromites at 4.2 K show two well developed sextets superposed with small difference of hyperfine fields (H hf) caused by Cr3?+? ions in two different magnetic sites. The values of the isomer shifts show that the charge states of Fe are Fe3?+? for all temperature range. Ni-chromites Mössbauer spectra below T N present aline broadening due to a Jahn–Teller distortion and show that spin structure behavior of Cr ions change from an incommensurate to a commensurate state.  相似文献   

18.
Single-phased nanocrystalline particles of pure and 10 % Ti 4+-doped perovskite-related YFeO 3were prepared via mechanosynthesis at 450°C. This temperature is ~150–350 °C lower than those at which the materials, in bulk form, are normally prepared. Rietveld refinements of the X-ray diffraction patterns reveal that the dopant Ti 4+ ions prefer interstitial octahedral sites in the orthorhombic crystal lattice rather than those originally occupied by the expelled Fe 3+ ions. Magnetic measurements show canted antiferromagnetism in both types of nanoparticles. Doping with Ti 4+ lowers the Néel temperature of the YFeO 3 nanoparticles from ~ 586 K to ~ 521 K. The Ti 4+-doped YFeO 3 nanoparticles exhibit enhanced magnetization and coercivity but less magnetic hyperfine fields relative to the un-doped nanoparticles. The 57Fe Mössbauer spectra show ~ 15 % of the YFeO 3 nanoparticles and ~22 of Ti 4+-doped YFeO 3 ones to be superparamagnetic with blocking temperatures < 78 K. The broadened magnetic components in the 57Fe Mössbauer spectra suggest size-dependent hyperfine magnetic fields at the 57Fe nuclear sites and were associated with collective magnetic excitations. The 57Fe Mössbauer spectra show the local environments of the Fe 3+ ions in the superparamagnetic nanoparticles to be more sensitive to the presence of the Ti 4+ ions relative to those in the larger magnetic nanoparticles.  相似文献   

19.
In recent years the synthesis of antiferromagnetic rings traced a path to the observation of interesting quantum coherence phenomena in heterometallic Single Molecule Magnets. Because of the presence of different magnetic centers, it is crucial to understand the distribution of the molecular spin on all the sites. 57Fe Mössbauer spectroscopy is an efficient and powerful technique to contribute to this knowledge in antiferromagnetic wheels containing iron ions. We analyze the Cr7FeII wheel: the Mössbauer line shape evolution of low temperature spectra (2.1 K) at different external fields is illustrated and the mean spin value of the iron ion is evaluated.  相似文献   

20.
The compound [Fe2L(H2O)4] (ClO4)4.H2O which contains pairs of Fe3+ ions within a binucleating macrocycle derived from Schiff base condensation of 2,6-diacetylpyridine and 1,3-diamino-2-hydroxy-propane has been studied by magnetic susceptibility measurements and57Fe Mössbauer spectroscopy between 4.2 K and 300 K, and its crystal structure determined. The spectra show relaxation effects at all temperatures. Spectra taken at 4.2 K in applied fields of about 3 T showed thatV zz is positive and η~0. The spectra were fitted using a stochastic model of a magnetic hyperfine field relaxing parallel to thez axis, giving relaxation times of 10?9?10?10 s.  相似文献   

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