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Magnetic and spectroscopic properties of the planar antiferromagnet K2FeF4 are determined by the Fe2+ ions at tetragonal sites. The two-dimensional easy-plane anisotropy exhibited by K2FeF4 is due to the zero field splitting (ZFS) terms arising from the orbital singlet ground state of Fe2+ ions with the spin S=2. To provide insight into the single-ion magnetic anisotropy of K2FeF4, the crystal field theory and the microscopic spin Hamiltonian (MSH) approach based on the tensor method is adopted. Survey of available experimental data on the crystal field energy levels and free-ion parameters for Fe2+ ions in K2FeF4 and related compounds is carried out to provide input for microscopic modeling of the ZFS parameters and the Zeeman electronic ones. The ZFS parameters are expressed in the extended Stevens notation and include contributions up to the fourth-order using as perturbation the spin-orbit and electronic spin-spin couplings within the tetragonal crystal field states of the ground 5D multiplet. Modeling of the ZFS parameters and the Zeeman electronic ones is carried out. Variation of these parameters is studied taking into account reasonable ranges of the microscopic ones, i.e. the spin-orbit and spin-spin coupling constants, and the energy level splittings, suitable for Fe2+ ions in K2FeF4 and Fe2+:K2ZnF4. Conversions between the ZFS parameters in the extended Stevens notation and the conventional ones are considered to enable comparison with the data of others. Comparative analysis of the MSH formulas derived earlier and our more complete ones indicates the importance of terms omitted earlier as well as the fourth-order ZFS parameters and the spin-spin coupling related contributions. The results may be useful also for Fe2+ ions at axial symmetry sites in related systems, i.e. Fe:K2MnF4, Rb2Co1−xFexF4, Fe2+:Rb2CrCl4, and Fe2+:Rb2ZnCl4. 相似文献
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The optical reflectivity of the red bronze K0.33MoO3 has been measured on single crystals in the spectral energy range between 0.03 and 12 eV at temperatures from 4 K to 300 K using polarized light. The optical constants have been determined by means of a Kramers-Kronig analysis; the data are interpreted that this compound is a 0.5 eV energy gap semiconductor with very strong anisotropy in the infrared and visible energy range. 相似文献
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C.M. Williams N.C. Koon J.B. Milstein 《Journal of Physics and Chemistry of Solids》1978,39(8):823-827
Room temperature magnetic anisotropy measurements have been made on a series of low anisotropy HoxTb1?xFe2 compounds, with 0.826 < x < 0.908, using torque magnetometry techniques. An analysis of the data using the conventional expansion of anisotropy energy in terms of the direction cosines proved inadequate because of the presence of higher order contributions to the anisotropy. When these contributions were included in the expansion, non unique anisotropy constants were obtained which were not consistent with the predictions of the single ion model. An analysis of the data using an expansion of the anisotropy in terms of an orthonormal set of functions, namely the cubic harmonics developed by Mueller and Priestly, proved more successful. The results showed that the two lowest order anisotropy constants, κ4 and κ6, both varied linearly with holmium concentrations as predicted by the single ion model; however, κ8, the next higher order term, was not consistent with the predicted behavior. The origin of this contribution is believed to be related to the magnetostriction. 相似文献
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A.V. Andreev 《Physica B: Condensed Matter》2009,404(19):2978-2980
A comparative study of magnetization in UFe6Al6 and LuFe6Al6 single crystals gives clear evidence for the magnetic state of uranium in UFe6Al6. Both compounds exhibit the easy-plane type of magnetic anisotropy, however, the anisotropy energy in UFe6Al6, characterized by the anisotropy constants K1=−7.3 MJ m−3 and K2=−1.25 MJ m−3 at 2 K, exceeds by an order of magnitude that in LuFe6Al6. Anisotropy within the easy plane in the ferromagnetic state and anisotropy in the paramagnetic range, both absent in LuFe6Al6, are observed in UFe6Al6. 相似文献
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The temperature dependence of the elastic constants of cubic K2Hg(CN)4 has been measured by optical Brillouin spectroscopy in the temperature range from 300-110 K. A decrease of all three elastic constants was found in agreement with the results of ultrasonic measurements. Raman measurements in the temperature range from 300-4 K revealed a splitting of the F2g modes corresponding to a trigonal distortion of the Hg(CN)4-tetrahedra in the low temperature phase. 相似文献
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建立了一种简便的、适用于磁畴模型应用的Tb0.3Dy0.7Fe2 合金本构参数辨识方法. 针对Tb0.3Dy0.7Fe2合金磁畴模型中本构参数不明确且直接实验测试困难的问题, 提出了一种数值计算与实验测试相结合的参数辨识方法. 采用坐标变换与绘制自由能等势曲线相结合的方法, 简化了载荷作用下Tb0.3Dy0.7Fe2 合金内磁畴角度偏转的数值计算, 研究了合金磁畴角度偏转模型的参数依赖性. 在此基础上, 结合简单的实验测试, 建立了Tb0.3Dy0.7Fe2合金各向异性常数K1 和K2、能量分布因子ω、晶轴取向分布的辨识及修正方法. 该方法能够简单、快速地完成Tb0.3Dy0.7Fe2 合金磁畴模型中本构参数的辨识, 对完善磁致伸缩材料磁畴偏转的数值计算模型非常有意义. 理论分析可为类磁致伸缩材料磁机耦合模型的建立、完善, 以及材料本构参数的辨识、获取提供参考. 相似文献
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The hyperfine fields of Cu2+ and F- ions nearest to a Zn2+ ion are measured by a spin echo method in a single crystal of K2Cu0.95Zn0.05F4. It is shown that the local symmetry due to the Jahn-Teller distortion is practically unaffected by the proximity of Zn2+ ions. 相似文献
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The spin-rotational Hamiltonian for an asymmetric-top molecule in a given vibrational level of an open-shell electronic state may contain more parameters than can be determined from the observed energy levels. This paper describes the reduction of the Hamiltonian by means of a unitary transformation to a form suitable for fitting to observed energies. It is shown that, for molecules of lower than orthorhombic symmetry, there are fewer determinable quadratic spin-rotation parameters than have been used previously. For example, for a molecule belonging to the group C8, there are four, not five, determinable spin-rotation constants, ?αβ. Similar indeterminacies exist among the quartic terms of the spin-rotation Hamiltonian. The case of a molecule of orthorhombic symmetry, for which there are six determinable quartic parameters, is considered in detail. The results are applied to the experimental data available on the spin-rotation splittings of the HO2 and NH2 radicals in their ground vibrational and electronic states. 相似文献
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Gang Luo 《Journal of Physics and Chemistry of Solids》2006,67(4):639-642
We present measurements of the paramagnetic susceptibilities of K3Pr2(NO3)9 and K3Sm2(NO3)9, cubic materials with rare earth sites having threefold rotational symmetry about (111). The rare earth environment resembles that of the Ln2Mg3(NO3)12·24H2O materials, and the magnetic susceptibilities show similarities but also interesting differences with Pr2Mg3(NO3)12·24H2O and Sm2Mg3(NO3)12·24H2O. Paramagnetic resonance experiments in K3La2(NO3)9 doped with these and several heavier lanthanides are also described and compared with theory. 相似文献
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本文研究了金属玻璃(Fe1-xCOx)78Si10B12的磁化感生各向异性、应变感生各向异性随成分和温度的变化。磁化感生各向异性常数Kum为正值,x=0.7时为最大;不可逆的应变感生各向异性常数Kusi为正值,x=0.5时为最大;可逆的应变感生各向异性常数Kusr除了x>0.975区均为负值,在x=0.7时为最大;感生各向异性常数在温度变化时与Msα成正比,α在3.4和7.5之间随成分和退火工艺而变化。用短程有序模型解释了部分实验结果。
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E.F. Steigmeier D. Baeriswyl G. Harbeke H. Auderset G. Scheiber 《Solid State Communications》1976,20(7):661-665
In previous work we have observed the amplitude mode of the charge density wave (CDW) in K2Pt(CN)4Br0.3?3.2H2O (KCP) by means of Raman scattering. New measurements made on deuterated material, K2Pt(CN)4Br0.3?3.2D2O (KCP1), show the same mode but shifted from 44 to 38 cm?1, maintaining the symmetry properties and temperature dependence of frequency and linewidth. This considerable isotope effect is interpreted in terms of a coupling of the CDW with the water stretching mode, which by the deuteration is shifted from 3494 cm?1 in KCP to 2560 cm?1 in KCP1 according to the change in atomic mass. Both of these modes exhibit A1(z) symmetry. At 5 K the resulting decoupled frequency of the CDW amplitude mode is 57 cm?1, and the coupling energy about 140 cm?1. A discussion of the temperature dependence of various important quantities is given. The present results show that the water molecules, which are located in between the Pt chains are strongly involved in the eigenvector of the CDW amplitude mode. 相似文献
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I. Ozier J. Schroderus S.-X. Wang G.A. McRae M.C.L. Gerry B. Vogelsanger A. Bauder 《Journal of Molecular Spectroscopy》1998,190(2):324-340
The pure rotational spectrum driven by the small distortion dipole moment perpendicular to the symmetry axis has been investigated between 8 and 18 GHz for CH3CF3in the ground vibrational state using a pulsed Fourier transform waveguide spectrometer. This molecule has been selected as a prototype for the case of a symmetric top with small (∼500 kHz) torsional energy splittings in the ground torsional state (ν6= 0). In this state, six (k± 3 ←k)Q-branch series have been measured for lower stateK= |k| between 3 and 8 with 27 ≤J≤ 75. For (ν6= 1), three series with lower stateKbetween 5 and 7 with 49 ≤J≤ 66 have been observed. In two of these series, the torsional fine structure extending over ∼6.8 MHz has been fully resolved. The (A1−A2) splitting has been measured in the (ν6= 0) series (K= 6 ← 3) for 37 ≤J≤ 74. The global data set of 443 frequencies included avoided-crossing molecular-beam splittings of Meerts and Ozier (1991.Chem. Phys.152, 241–259) and mm-waveR-branch measurements of Bocquetet al.(1994.J. Mol. Spectrosc.165, 494–499). In a weighted least-squares analysis, a good fit was obtained by varying 18 parameters in a Hamiltonian that represented both the torsional effects and the sextic splittings. Effective values have been determined for both rotational constants, eight torsional parameters including the barrier height, six diagonal centrifugal distortion constants, and two centrifugal distortion constants (? and ?J) that characterize the (Δk= ±3) matrix elements. The difficulties are discussed that arise in defining a unique model for the torsional terms in the Hamiltonian when a high barrier symmetric top is investigated by distortion moment spectroscopy. The redundancies are investigated that exist in the quartic and sextic Hamiltonian for a near-spherical top such as CH3CF3. 相似文献
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We report magnetic properties of silica-coated CoFe2O4 nanoparticles (about 32 nm) in a wide temperature range (4-700 K). Coating CoFe2O4 nanoparticles with amorphous silica yields an assembly of noninteracting single-domain particles with cubic magnetocrystalline anisotropy. We find that the reduced remanence is about 0.81-0.82 at low temperatures (?100 K), very close to the theoretical prediction (0.83) for cubic anisotropy. The room-temperature anisotropy constant K1 inferred from the data is also in quantitative agreement with the bulk value (1.8×106 erg/cm3). The current work thus provides a quantitative test for a theory of noninteracting single-domain particles with cubic anisotropy. 相似文献
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Arthur Maki Thomas A. Blake Robert L. Sams Nicolae Vulpanovici Jeffrey Barber Engelene T.H. Chrysostom Tony Masiello Joseph W. Nibler Alfons Weber 《Journal of Molecular Spectroscopy》2001,210(2)
New measurements are reported for the infrared spectrum of sulfur trioxide, 32S16O3, with resolutions ranging from 0.0015 cm−1 to 0.0025 cm−1. Rovibrational constants have been measured for the fundamentals ν2, ν3, and ν4 and the overtone band 2ν3. Comparisons are made with the earlier high-resolution measurements on SO3, and the high correlation among some of the constants related to the Coriolis coupling of the ν2 and ν4 levels is discussed in order to understand the areas of disagreement with the earlier work. Splittings of some of the levels are observed and the splitting constant for K=3 of the ground state is determined for the first time. Other observed splittings include the K=1 levels of 2ν3 (l=2), the K=2 levels of ν3 and ν4, and the K=3 levels of ν2. The analysis shows that there are level crossings between the l=0 and l=2 states of 2ν3 that allow one to determine the separation of the subband centers for these two states even though access to the l=0 state from the ground state is electric-dipole forbidden. This is a generalized phenomenon that should be found for many other molecules with the same symmetry. The l-type resonance constant, q3, that causes the splitting of the l3=±1, k=±1 levels of ν3 also couples the l3=0 and 2 states of 2ν3. 相似文献