Analysis of antiferromagnetic resonance in KNiF3

We have compared theoretical calculations of the temperature dependence of the antiferromagnetic resonance field for KNiF₃, a cubic crystal, with the experimental data obtained by other authors. We have discussed the applicability to the cubic case of Kittel's equations for a uniaxial system. We have used experimental values from the literature for the magnetic susceptibilities and anisotropy in the expression for the antiferromagnetic resonance field.     

Light scattering from two-magnon modes in K2NiF4

Measurements of Raman scattering from two magnon excitations in the two dimensional antiferromagnet K₂NiF₄ are extended to 275°K. The zeroth frequency moment of the magnon signal has a temperature dependence essentially the same as that found in the three dimensional antiferromagnet, NiF₂. No indications of critical behavior are apparent in the first frequency moment for K₂NiF₄ in contrast to the case of three dimensional antiferromagnets.     

Sound propagation in the two dimensional magnetic system K2NiF4

We have measured the classic constants C₁₁, C₃₃, C₅₅ and C₆₆ in K₂NiF₄ as a function of temperature between 4.2 and 200 K. A small velocity and attenuation anomaly was observed in the C₁₁ mode at T_N = 97.2 K.     

K2NiF4型Sr2CrO4的磁电性质研究

以SrO和CrO₂为原料, 在高温高压的条件下直接反应生成纯相的K₂NiF₄结构的Sr₂CrO₄多晶样品. 结构用粉末X射线衍射及GSAS精修表征. 磁化率测试显示样品存在一个弱的反铁磁相变, 奈尔温度为T_N=95 K. 在奈尔温度以上, 磁化率随温度的变化遵循居里-外斯定律. 对样品进行了电阻测试, 结果显示了样品的绝缘特性.     

New perovskite related-compounds of Ru(V) in K2NiF4 type structure

The preparation of the new K₂NiF₄-type compounds, Sr₂Co_0.5Ru_0.5O₄, Sr₂Ni_0.5Ru_0.5O₄ and Sr₂Ga_0.5Ru_0.5O₄ by direct solid state synthesis and the subsequent characterization by powder X-ray diffraction measurements are described. From Rietveld refinements, we found that the compounds have a K₂NiF₄-type structure with the symmetry of space group I4/mmm. It was found that in these compounds, the substituted trivalent metal ions (M=Co, Ni, and Ga) and the Ru ions are disordered over the octahedral B sites of the K₂NiF₄ structure. The octahedral Ru-O environment is less elongated in the apical direction in these compounds than in the Sr₂RuO₄ compound. We also found that the octahedron in Sr₂Ga_0.5Ru_0.5O₄ is more symmetric than that of Sr₂Co_0.5Ru_0.5O₄ and Sr₂Ni_0.5Ru_0.5O₄. The Ru K-edge X-ray absorption measurements showed that Ru ions were in a pentavalent oxidation state.     

Soft modes below the incommensurate transition in K2SeO4

A coordinated series of Raman and Brillouin scattering measurements were carried out in K₂SeO₄ with emphasis on temperatures near and below the incommensurate structural phase transition (T_i=129 K). Below the lock-in phase transition (T_c=99 K) Raman scattering from both the amplitude mode and the phase mode analog was observed. However, only the amplitude mode could be followed into the incommensurate phase. Details of the amplitude mode frequency and damping are reported for temperatures considerably closer to T_i than previously possible. Our results do not confirm the diverging linewidth extrapolated from earlier Raman work. We also report here the first Brillouin scattering results in K₂SeO₄. Although substancial interaction effects between the acoustic phonons and the soft amplitude mode are evident near T_i, the coupled mode lineshapes can be well described without the introduction of a relaxing self energy for the soft mode. Finally, limits on the characteristics of the phason are drawn from our failure to observe it directly in the incommensurate phase.     

Elastic anomaly in K2ZnCl4 around the normal-incommensurate-commensurate phase transition points

The ultrasonic velocities in K₂ZnCl₄ were measured as functions of temperature. At the incommensurate-commensurate phase transition point the velocity of the c₅₅ mode showed a clear anomaly, whereas anomalies were hardly observable in all other modes. The results are analyzed in terms of a phenomenological theory.     

First order antiferromagnetic phase transition in MnS2

The antiferromagnetic structure of MnS₂ has been re-examined by neutron diffraction from a single crystal. The phase transition has been found to be of the first order without any detectable thermal hysteresis. Application of uniaxial stress tends to convert the first order transition into a second order one.     

Hyperfine interactions in Zn-doped K2CuF4

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 K₂Cu_0.95Zn_0.05F₄. It is shown that the local symmetry due to the Jahn-Teller distortion is practically unaffected by the proximity of Zn²⁺ ions.     

Raman spectra of K2CuF4

The crystal structure of K₂CuF₄ has been studied by means of Raman scattering. The structure is found to belong to the space group D_4h⁵ rather than D_4h¹⁷ of K₂NiF₄ between 2 and 800 K because of the distortion arising from the “orbital ordering effect”.     

Metastable chaotic state in K2ZnCl4

The ³⁵Cl NQR frequencies of K₂ZnCl₄ have been measured close to the incommensurate-commensurate transition. A calculation of the temperature dependence of the soliton density n_s from the NQR data showed that in K₂ZnCl₄ close to T_c exists a metastable chaotic state.     

Brillouin spectroscopy in K2Ba(NO2)4

The temperature dependence of elastic stiffnesses of K₂Ba(NO₂)₄ is investigated in the range - 140 to + 160°C, in which two phase transitions have been reported. Marked anomalies appear at the lower transition, in contrast with continuous variations through the upper transition. Results are compared to those obtained near the upper transition by an ultrasonic method and they are qualitatively discussed.     

Critical behaviour of the two-dimensional ising antiferromagnets K2CoF4 and Rb2CoF4

The studies have been performed by means of neutron scattering. We report here the first experimental verification of the theoretical predictions concerning temperature dependence of the long range order parameter of two-dimensional Ising systems, giving the values B = 1·16±0·03 and β = 0·119±0·008 for the critical parameters. Also the parameters for the inverse correlation length and the staggered susceptibility were determined, with exponents v = 0·89±0·1 and γ = 1·34±0·22. It was discovered that frozen-in states of stacking of the two-dimensional planes appeared upon quick cooling through the ordering temperature.     

Magnetic excitations in the two dimensional planar antiferromagnets K2FeF4 and Rb2FeF4

The magnetic excitation spectrum of K₂FeF₄ and Rb₂FeF₄, two K₂NiF₄-structure planar antiferromagnets with rather large anisotropy and spins perpendicular to the c-axis, has been measured by Raman and FIR-spectroscopy. One of the two predicted one-magnon transitions and the two-magnon mode have been observed in K₂FeF₄ (Rb₂FeF₄) at 48.5 cm^-1 (37.6 cm^-1) and 182.0 cm^-1 (160.5 cm^-1) respectively. The magnetic field and temperature dependence of the spectra are reported too. The data are discussed on the basis of an easy plane spin model Hamiltonian. In K₂FeF₄: Mn²⁺ a low lying magnetic impurity mode is observed at 40.5 cm^-1.     

Critical behaviour of the linear birefringence in 3d-Heisenberg antiferromagnets : RbMnF3, KNiF3 and KCoF3

The linear birefringence of stress induced single antiferromagnetic T-domains of RbMnF₃, KNiF₃ and KCoF₃ has been measured in the vicinity of T_N. We deduce the critical behaviour in such 3d-Heisenberg systems, showing a symmetry breaking at the transition involving a unique wave vector of the order parameter in the Brillouin zone. The critical exponent $\text{β}$ of the linear birefringence has been found to be larger than 2β, in agreement with the theoretical predictions of G. Gehring.     

Two magnon light scattering in K2MnF4

The light scattering spectra of the two dimensional Heisenberg antiferromagnet K₂MnF₄ are reported. At low temperatures a two magnon band is observed and four bands due to phonons as well.     

Localized magnon gap modes in the 2-d Ising antiferromagnets K2CoF4 and Rb2CoF4

The defect (Mn²⁺,Ni²⁺,Fe²⁺) induced magnon gap modes in the layered antiferromagnets K₂CoF₄ and Rb₂CoF₄ were investigated with the methods of FIR absorption-and IR emission spectroscopy. The anisotropic exchange-parameters describing the strongly localized Mn²⁺ spin excitations far below the host lattice magnon band and the Ni²⁺ excitations in the vacinity of this band are presented. In the diluted system K₂Co_1-cMn_cF₄ localized Mn²⁺ cluster modes up to about C≈0.1 were observed. The excitation energy of these modes can only be explained by assuming an anisotropic Mn²⁺-Mn²⁺ exchange which is in contrast to the pure isomorphous system K₂MnF₄. In the spin mismatch system K₂CoF₄: Fe the magnetic moments of the isolated Fe²⁺ impurities are pulled from the plane perpendicular to the c-axis and aligned parallel to the easy axis of the magnetic crystal.     

Jahn-Teller band transition in La3S4 and La3Se4

La₃S₄ and La₃Se₄ undergo a cubic to tetragonal phase transformation at a temperature of 103 and 70 K respectively, the c/a ratio is 0.984 for La₃S₄ and 0.987 for La₃Se₄. In these compounds the conduction electron Fermi energy happens to be close to a band structure anomaly which drives the phase transition. We find some indication, that the anomaly might be of ?-type.     

Behavior of the antiferromagnetic phase transition near the fermion condensation quantum phase transition in YbRh2Si2

Low-temperature specific-heat measurements on YbRh₂Si₂ at the second order antiferromagnetic (AF) phase transition reveal a sharp peak at TN=72 mK. The corresponding critical exponent α turns out to be α=0.38, which differs significantly from that obtained within the framework of the fluctuation theory of second order phase transitions based on the scale invariance, where α?0.1. We show that under the application of magnetic field the curve of the second order AF phase transitions passes into a curve of the first order ones at the tricritical point leading to a violation of the critical universality of the fluctuation theory. This change of the phase transition is generated by the fermion condensation quantum phase transition. Near the tricritical point the Landau theory of second order phase transitions is applicable and gives α?1/2. We demonstrate that this value of α is in good agreement with the specific-heat measurements.