Critical line broadening of the EPR in the two-dimensional antiferromagnet crystals Rb2MnCl4 and Rb2Mn0,8Cd0,2Cl4

The EPR spectrum of quasi-two-dimensional antiferromagnets Rb₂Mn_xCd_1?xCl₄ (x=1,0; 0,8) has been studied in a critical temperature range. Two theoretical approaches - the scaling theory and the soliton's theory - are used to explain experimental data on temperature of the EPR linewidth. In the first interpretation critical exponents are determined. For both crystal two temperature regions with different critical exponents are found. It is shown that the soliton's theory with an anomaleous great excitement energy describes the experimental data satisfactory.     

Thermoremanent magnetization in Rb2Mn(1-x)CrxCl4 spin-glass

Time dependence of thermoremanent magnetization (TRM) in a new spin-glass, Rb₂Mn_(1-x)Cr_xCl₄ is measured at temperatures below the freezing temperature. The result shows that long time behavior of the TRM obeys a power law, M(t) = Ct^?A. It is shown from the analysis of the experiment that there is a possibility of the presence of a critical temperature.     

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.     

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.     

Antiferromagnetic resonance in Rb2Mn(1−x)CrxCl4: A randomly mixed insulating antiferromagnet and ferromagnet

Electron spin resonance experiments at submillimeter and millimeter wavelengths have been performed on the random mixture, Rb₂Mn_(1-x)Cr_xCl₄ of an insulating antiferromagnet Rb₂MnCl₄ and an insulating ferromagnet Rb₂CrCl₄. From the antiferromagnet resonance in the Mn-rich concentrations, the antiferromagnetic exchange field is shown to become small with Cr concentration. Thus, a competition between the antiferromagnetic and ferromagnetic exchange interactions really exists in this mixed system.A competition of the uniaxial anisotropy of Rb₂MnCl₄ with the planar one of Rb₂CrCl₄ has also been found.     

Neutron diffraction and magnetic measurements of polycrystalline NH4MnCl3

Neutron diffraction and magnetic susceptibility measurements show NH₄MnCl₃ to be an antiferromagnet of type G with T_N ∼ 105°K. The low temperature patterns reveal a tetragonal splitting and superlattice lines which were accounted for by assuming the space group to be P bnm.     

Structure and magnetic order of Cr-rich Rb2Cr1-xMnxCl4 crystals

The distorted K₂NiF₄-structure and the magnetic behaviour of the quasi two-dimensional magnetic system Rb₂Cr_1-xMn_xCl₄ (0 ? x ? 0.5) are studied by neutron diffraction and magnetic measurements. Strong correlations between ferromagnetic coupling and cooperative Jahn—Teller order are indicated by their occurence in the same concentration range 0 ? x ? 0.41.The percolation threshold x_F near x = 0.41 and the x, T-dependence of the para- to ferro-magnetic phase boundary are quite similar to that found in systems with non-magnetic impurities. Further we report the magnetic moment magnitudes in this percolative system.     

Selection rules for superstructures in thiourea,Rb2ZnBr4 and Rb2ZnCl4

This paper concerns the superstructures to which a modulated structure locks in. For thiourea, all observed rational values of $\text{γ (}\text{q}\text{= γ}\text{c}{}^1\text{)}$ belong to a certain type of fractions, namely - if we put $\text{γ =}\text{e}\text{v}$ - those with both u and v odd. In Rb₂ZnBr₄ and Rb₂ZnCl₄, published data point strongly to the existence of superstructures which so far had been regarded as incommensurate, but which turn out to yield values $\text{u}\text{v}$ also obeying the above parity conditions. Such conditions can be explained by a new hypothesis, viz. that the point group of the lock-in phase is identical to the three-dimensional part of the point group of the adjoining incommensurate phase.     

Magnetic resonances in (CH3NH3)2MnCl4

We have studied the magnetic excitations of (CH₃NH₃)₂MnCl₄ in the antiferromagnetic and in the spin-flop regimes by means of magnetic resonance in the millimeter range (60–100 GHz). Rather odd line shapes of the resonance absorption line for narrow lines are explained as interference effects between the resonant and the non-resonant circular wave in the sample. For the antiferromagnetic resonance (AFMR) and for the paramagnetic resonance (EPR, above the Néel temperature), we have also studied the line width as a function of temperature.     

四氯乙烯的同步辐射光电离研究

利用VUV同步辐射光源和反射式飞行时间质谱仪，在超声冷却条件下对四氯乙烯(C₂Cl₄)进行了光电离研究，通过测量各离子的光电离效率(PIE)曲线，得到了C₂Cl₄的电离势IP(C₂Cl₄) =(9.36±0.05)eV及C₂Cl₄光解离碎片离子C₂Cl₃⁺，C_{关键词： 真空紫外光电离 离子出现势 电离势 四氯乙烯}     

Structural information from EPR powder spectra of Mn(II)-doped Rb2MgCl4, Rb2MgCl3Br and Rb2MgCl2Br2

The structure of the compounds Rb₂MgCl₄, Rb₂MgCl₃Br and Rb₂MgCl₂Br₂ has been determined to be the tetragonal K₂NiF₄ structure. EPR spectra at X and Q-band frequencies of the polycrystalline samples of the Mn(II)-doped compounds, indicate that the Br^? ions prefer to order at special sites of the structure, as concluded from the fact that only octahedral groups [MgCl₆] and tetragonal groups [MgCl₄Br₂] are found.     

Synthesis and crystallographic studies of garnet-type AgCa2Mn2V3O12 and NaPb2Mn2V3O12

High-purity powder specimens of AgCa₂Mn₂V₃O₁₂ and NaPb₂Mn₂V₃O₁₂ have been successfully synthesized by solid-state chemical reaction. The Rietveld refinements from X-ray powder diffraction data verified that these compounds have the garnet-type structure (space group , No. 230) with the lattice constant of a=12.596(2) Å for AgCa₂Mn₂V₃O₁₂ and a=12.876(2) Å for NaPb₂Mn₂V₃O₁₂. Calculation of the bond valence sum supported that Mn is divalent and V is pentavalent in these garnets. Estimation of the quadratic elongation and the bond angle variance showed that the distortions of the MnO₆ octahedra and the VO₄ tetrahedra are significantly suppressed. Our new results of AgCa₂Mn₂V₃O₁₂ and NaPb₂Mn₂V₃O₁₂ are compared to those of AgCa₂M₂V₃O₁₂ and NaPb₂M₂V₃O₁₂ (M=Mg, Co, Ni, Zn).     

Anisotropic and large low-field magnetic entropy change in a La4/3Sr5/3Mn2O7 single crystal

We have studied the magnetocaloric effect (MCE) in a bilayered La_4/3Sr_5/3Mn₂O₇ single crystal with applied field along both ab-plane and c-direction. Due to the quasi-two-dimensional structure, the crystal exhibits a strong anisotropy in the MCE. The difference of magnetic entropy change between two crystallographic directions depends on external magnetic fields and has a maximum of 2 J/kg K. A large low-field magnetic entropy change, reaching 3.2 J/kg K for a magnetic field change of 15 kOe, is observed when the applied field is along ab-plane. This large low-field magnetic entropy change is attributed to the rapid change of magnetization in response to external magnetic fields in the easy magnetizing plane.     

Absolute Raman intensities of CH4, CH3D,CH2D2, CHD3, and CD4

Measurements of the absolute vibrational Raman intensities and depolarization ratios for the fundamental and some overtone and combination bands of CH₄, CH₃D, CH₂D₂, CHD₃, and CD₄ are reported. Experimental aspects of these measurements are discussed. The experimental data conform satisfactorily to all isotope intensity sum rules. The measured intensities and depolarization ratios, together with the vibrational potential function for CH₄, make possible the calculation of the four independent parameters of the isotopic invariant quantities $\text{α}{}^{\mathrm{S}}\text{= |}\text{?α}\text{?S}\text{|}$. The results deduced from these agree with all 36 experimentally observed values. Values of electro-optical parameters for the CH bond are calculated and discussed.     

Geometric shielding corrections for total cross section calculations of electron scattering by CH4, C2H6, C2H3F3, C2H4, C2F4, C2Cl4 and C2Cl2F2 from 30–5000?eV

To quantify the changes in the geometric shielding effect in a molecule as the incident electron energy varies, an empirical fraction, which represents the total cross section contributions of shielded atoms in a molecule at different energies, is presented. Using this empirical fraction, the total cross sections for electron scattering by CH₄, C₂H₆, C₂H₃F₃, C₂H₄, C₂F₄, C₂Cl₄ and C₂Cl₂F₂ are calculated over a wide energy range from 30 to 5000 eV by the additivity rule model at the Hartree-Fock level. The quantitative total cross sections are compared with those obtained by experiment and other theories where available. Good agreement is attained above 100 eV.     

Chlorine K X-ray absorption-edge structures of CIS-[Pt(NH3)2Cl2], trans-[Pt(NH3)2Cl2], trans-[Pd(NH3)2Cl2] and (NH4)2PdCl4

The K absorption-edge spectra of the ligand chlorine ion in square-planar complex compounds cis- and trans-[Pt(NH₃)₂Cl₂], trans-[Pd(NH₃)₂Cl₂], and (NH₄)₂PdCl₄ are reported and discussed in connection with the chlorine K absorption spectra of K₂PtCl₄ and K₂PdCl₄, reported previously. The observed chemical shift of a white line at the absorption threshold is interpreted in terms of the difference of the ligand-field splitting of electronic states for metal ions. The white line is attributed to the electronic transition from the Cl^? ls level to the lowest unoccupied antibonding molecular orbital (MO), which is specified by a $\text{MO}\text{b}{}_{\mathrm{1g}}\text{(σ}{}^1\text{)}$ in the square-planar complex with D_4h symmetry. The other absorption structures are regarded as continuum “shape resonances” of the outgoing electron trapped by the cage of the surrounding atoms. The effect of geometrical isomerism is found in the chlorine K absorption spectra of cis- and trans-[Pt(NH₃)₂Cl₂].     

High-pressure Raman spectroscopic studies on orthophosphates Ba3(PO4)2 and Sr3(PO4)2

By using diamond anvil cell (DAC), high-pressure Raman spectroscopic studies of orthophosphates Ba₃(PO₄)₂ and Sr₃(PO₄)₂ were carried out up to 30.7 and 30.1 GPa, respectively. No pressure-induced phase transition was found in the studies. A methanol:ethanol:water (16:3:1) mixture was used as pressure medium in DAC, which is expected to exhibit nearly hydrostatic behavior up to about 14.4 GPa at room temperature. The behaviors of the phosphate modes in Ba₃(PO₄)₂ and Sr₃(PO₄)₂ below 14.4 GPa were quantitatively analyzed. The Raman shift of all modes increased linearly and continuously with pressure in Ba₃(PO₄)₂ and Sr₃(PO₄)₂. The pressure coefficients of the phosphate modes in Ba₃(PO₄)₂ range from 2.8179 to 3.4186 cm⁻¹ GPa⁻¹ for ν₃, 2.9609 cm⁻¹ GPa⁻¹ for ν₁, from 0.9855 to 1.8085 cm⁻¹ GPa⁻¹ for ν₄, and 1.4330 cm⁻¹ GPa⁻¹ for ν₂, and the pressure coefficients of the phosphate modes in Sr₃(PO₄)₂ range from 3.4247 to 4.3765 cm⁻¹ GPa⁻¹ for ν₃, 3.7808 cm⁻¹ GPa⁻¹ for ν₁, from 1.1005 to 1.9244 cm⁻¹ GPa⁻¹ for ν₄, and 1.5647 cm⁻¹ GPa⁻¹ for ν₂.     

Magnetic resonance study of the magnetic structures of Rb2MnxCr1−xCl4, a random mixture of a ferromagnet and an antiferromagnet

We have studied samples of Rb₂Mn_xCr_1?xCl₄ with various concentrations x by magnetic resonance in the millimeter wave range. This mixed crystal system is of interest because of completing exchange interactions, in addition to competing anisotropies. One of the end members (Rb₂MnCl₄) is an easy-axis antiferromagnet while the other (Rb₂CrCl₄) is an easy-plane ferromagnet. Our experiments have been performed for different configurations in order to obtain information about the magnetic structure of the mixed crystal in the corresponding concentration range. On the Mn-rich site, this structure changes already at about 5% Cr²⁺ from an easy-axis antiferromagnet to an easy-plane antiferromagnet. With further increasing Cr²⁺ concentration, our results indicate an increasing ferromagnetic component which finally (Cr²⁺ concentration more than 60%, x ? 0.4) leads to a predominantly ferromagnetic order on the Cr-rich side.