Evidence for the spin-dependent scattering of conduction electrons on Mn2+ ions in Hg1−xMnxTe and Cd1−xMnxSe mixed crystals

Changes in the resistivity of Hg_1?xMn_xTe and Cd_1?xMn_xSe mixed crystals associated with paramagnetic resonance of the Mn²⁺ ions have been observed at liquid helium temperature in a strong magnetic field. The effect was recorded by monitoring the submillimeter radiation induced photoconductivity in a swept magnetic field. An increase in the resistivity associated with EPR of the Mn²⁺ ions is interpreted in terms of the spin- dependent scattering of electrons on magnetic impurities, the spins of which are selectively depolarised by means of paramagnetic resonance. Some additional effects influencing the experiments are also discussed.     

Crystal field parameters and energy level structure of the MnO4 tetroxo anion in Li3PO4, Ca2PO4Cl and Sr5(PO4)3Cl crystals

A comparative study concerning the electronic structure of the Mn⁵⁺ ion in the Li₃PO₄, Ca₂PO₄Cl, Sr₅(PO₄)₃Cl host lattices has been carried out in the framework of the exchange charge model. The crystal field parameters have been evaluated using the structural data as the only input information. The 10 K absorption spectra of the investigated compounds have been measured in order to verify the correspondence between experimental and calculated energy levels. A systematic trend of the crystal field splitting of the most intense transitions has been evidenced and discussed by considering the symmetry properties of the coordination polyhedra around Mn⁵⁺.     

169Tm Mössbauer effect and magnetic study of Tm6Mn23 and its ternary hydride

The magnetic properties and the lattice constants of Tm₆Mn₂₃ were determined before and after hydrogen absorption. The compound Tm₆Mn₂₃ is ferrimagnetic with an ordering temperature T_c = 404 K. After hydrogen absorption the magnetization is strongly reduced and does not point to the occurrence of magnetic ordering. The strongly increasing hyperfine splitting observed by means of ¹⁶⁹Tm Mössbauer spectroscopy in the hydride for temperature below 60 K, however, shows that the Tm sublattice becomes magnetically ordered after H₂ absorption as well. In uncharged and charged Tm₆Mn₂₃ the values of the Tm moments are close to the free ion values.     

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.     

Electron paramagnetic resonance in the system CaO-SiO2-Al2O3 containing sulfur

An EPR absorption was detected in the system CaO-SiO₂-Al₂O₃ doped with sulfur. The signal consisted of six isotropic hyperfine lines and demonstrated isotropic fine structure and forbidden doublets. The signal was attributed to an Mn²⁺ impurity displacing Ca²⁺ in fine CaS crystallites formed in the matrix of the ternary system. The spectrum was well accounted for with the parameters g = 2.0021 ± 0.0001 and A = ?77.1 ± 0.6 × 10^?4 cm^?1. Sample preparation conditions did not affect the hyperfine splitting, although the fine structure and forbidden lines proved to be dependent on the conditions of preparation. It is suggested that the appearance of the fine structure is a result of the second effect of the hyperfine structure when the cubic field parameter a approaches zero and, consequently, the structure is free of superposition caused by an anisotropic shift determined by a. We ascribe the change in fine structure to the variation in a and discuss the nature of the energy splitting of the ${}^6\text{S}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}$ state in a cubic field. We also note a correlation between the fine structure and the forbidden lines. This finding suggests that a is not necessarily specific to the host lattice and, furthermore, that the consideration of superposition of axial or lower symmetry upon the original cubic field of the central Mn²⁺ ion is vital for the determination of a.     

Mn activated MgSrAl10O17 green-emitting phosphor—A luminescence and EPR study

This paper reports on the luminescence and electron paramagnetic resonance (EPR) investigations on MgSrAl₁₀O₁₇:Mn²⁺ green-emitting phosphor. Single-phase MgSrAl₁₀O₁₇ was successfully synthesized by the one-step solution combustion route without the need for post-annealing at a higher temperature. Crystallization of the powder was confirmed by X-ray diffraction. The luminescence of Mn²⁺- activated MgSrAl₁₀O₁₇ shows a strong green-emission peak around 515 nm due to the ⁴T₁→⁶A₁ transition of Mn²⁺ ions under the excitation (453 nm). The EPR spectra of Mn²⁺ ions exhibit a sextet hyperfine structure centered at g ≈1.995. The Mn²⁺ ion occupies Mg sites which are in tetrahedral symmetry. The magnitude of the hyperfine splitting (A) indicates that Mn²⁺ is in a moderately ionic environment. The number of spins participating in resonance (N), the paramagnetic susceptibility (χ) and the zero-field splitting parameter (D) have been evaluated and discussed.     

Exciton dispersion in MnI2 and MnBr2

The line shape of some of the optical d-d transitions in MnI₂ and MnBr₂ is asymmetric and depends strongly on temperature and magnetic field strength. It is shown that these effects are due to the hopping of excitons from one Mn²⁺ ion to another. The hopping integral depends strongly on the correlation between the directions of the spins of the two ions involved. The line shape in the magnetically ordered crystals depends in a sensitive way on the type of magnetic order. We also present a simple method to calculate the line shape in crystals where the magnetic moments are not fully ordered.     

Tm Mössbauer effect and magnetic study of Tm6Mn23 and its ternary hydride

The magnetic properties and the lattice constants of Tm₆Mn₂₃ were determined before and after hydrogen absorption. The compound Tm₆Mn₂₃ is ferrimagnetic with an ordering temperature T_c = 404 K. After hydrogen absorption the magnetization is strongly reduced and does not point to the occurrence of magnetic ordering. The strongly increasing hyperfine splitting observed by means of ¹⁶⁹Tm Mössbauer spectroscopy in the hydride for temperature below 60 K, however, shows that the Tm sublattice becomes magnetically ordered after H₂ absorption as well. In uncharged and charged Tm₆Mn₂₃ the values of the Tm moments are close to the free ion values.     

Schottky-like anomaly in the low-temperature specific heat of single-crystal NdMnO3

The specific heat of single-crystal NdMnO₃ was investigated from 2 to 20 K under different magnetic fields up to 8 T. All the specific heat data show a Schottky-like anomaly, which becomes more indistinctive as increasing magnetic field. The experiment data were successfully fitted by taking into account factors such as crystal-field splitting, the two-level Schottky anomaly, the lattice vibration, and type-A antiferromagnetic (A-AF) spin waves. It was found that the splitting of the ground state doublet of Nd³⁺ ion increases linearly with magnetic field. The above phenomena can be interpreted in terms of the model of unchanged effective molecular field at Nd³⁺ site caused by the ferromagnetic component of A-AF structure of Mn spins. This ferromagnetic component is likely caused by the GdFeO₃-type octahedron rotation. In addition, it was also found that the magnetic field increases the spin-wave stiffness coefficient, but reduces the Debye temperature.     

Magnetic field effects on the fluorescence of Cr3+ in GdAlO3

The fluorescence spectrum of Cr³⁺ in GdAlO₃ has been examined at 4.2 K as a function of magnetic field up to 60 kG. The resulting splitting of the ²E → ⁴A₂ emission lines are explained in terms of a modified molecular field approximation, which incorporates the effect of the spin fluctuations. The exchange constant in the relaxed excited state is found to be 1.2 cm^-1, which differs from that reported from absorption data. It is suggested that the difference may be related to the Frank-Condon effect.     

Zeeman effect on the 4E level of Mn2+ in ZnS

The fine structure lines of the ⁴E level of Mn²⁺ in ZnS have been studied under a high magnetic field. Experiments were performed with the magnetic field parallel to the [111]_W crystallographic axis. The computed positions and intensities for polarized and non-polarized light are in agreement with the experiments.     

EPR and luminescence of Mn2+ in MgF2 single crystals

EPR spectra of Mn²⁺ in MgF₂ crystals grown by the Bridgman technique were measured at 300 and 20 K. Application of the superposition model to the zero field splitting (ZFS) patterns indicates complete absence of dynamic contributions to the ZFS. The luminescence spectra are also in accord with substitutional incorporation of Mn²⁺.     

Etude par diffraction neutronique de l'ilmenite ferrimagnetique NiMnO3

The magnetic structure of ferrimagnetic ilmenite Ni²⁺Mn⁴⁺O₃ has been investigated by neutron diffraction. Below the Curie temperature (164°C), the spins are oriented into two kinds of ferromagnetic planes perpendicular to the [111] rhomboedral axis, one containing Mn⁴⁺ and the other Ni²⁺ cation. Two successive planes are coupled antiferromagnetically. The experimental magnetic moments are respectively found equal to 1.8 and 2.2 μ_B for Ni²⁺ and Mn⁴⁺ at room temperature. The positional atomic parameters have been redetermined from nuclear diffraction data taken above the Curie temperature.     

EPR study on Mn2+-Cu2+ and Ni2+-Cu2+ mixed pairs

An EPR study at X- and Q-band frequencies has been made on mixed metal pairs Mn²⁺-Cu²⁺ and Ni²⁺-Cu²⁺ obtained by doping the dimer complex C₅H₅NO CuCl₂ · H₂O. Available experimental data have been confirmed and extended, particularly as regards the characteristic directions of the various magnetic tensors. The qualitative behaviour of the spectra and the somewhat singular values of the magnetic parameters can be well-described on the basis of a theoretical model in which a very strong “cosine” interaction between the total electronic spins is assumed. From the model some interesting new aspects emerge, concerning the relations between pairs and single-ion EPR parameters.     

Characterization of the 2D antiferromagnets Rb2MnCl4 and Rb3Mn2Cl7 : Optical,Raman and magnetic circular dichroism studies

Below T_N, the site symmetry at the Mn²⁺ ion is centrosymmetric (Rb₂MnCl₄) and non-centrosymmetric (Rb₃Mn₂Cl₇) respectively. As a result, one expects the appearance of magnetic dipole or electric dipole exciton origins in the optical spectra. These were clearly seen via polarized absorption and magnetic circular dichroism measurements through the 4T₂(D) band. The zone edge magnon frequencies are found to be 80 cm^?1 (Rb₂MnCl₄) and 90 cm^?1 (Rb₃MnCl₂in7). The two compounds are also easily distinguished through their room temperature axial absorption (⁴T₂ (G) band) and Raman spectra. Low temperature data indicate that the tetragonal field plays an important role.     

Spectre d'absorption et effet Zeeman de l'ion Mn2+ dans un sulfate acide de manganese et de potassium MnK4H2(SO4)4, 2H2O a basse temperature

We present aborption spectra of an oriented single crystal of MnK₄H₂(SO₄)₄, 2H₂O at temperatures between 20 and 1.6 K. This salt has orthorhombic symmetry and gives, both in the visible and ultraviolet regions, an absorption spectrum which changes considerably when the temperature decreases from 20 to 4.2 K. The spectrum has sharp lines at 1.6 K in the two absorption regions corresponding to teh excited levels ⁴A₁⁴E(⁴G) and ⁴T₂(⁴D). A study has been made of the Zeeman splitting of these sharp lines; a discontinuity has been observed in the Zeeman splitting as a function of magnetic field at 1.6 K. This discontinuity is a consequence of a magnetically-ordered phase.     

Y3Fe5-xMnxO12的磁结构和磁性能

对多晶Y₃Fe₃Fe_5-xMn_xO₁₂(x=0.05和0.09),得到300K下的中子衍射曲线。发现当x=0.05时,Mn³⁺离子占据16a和24d位置的几率分别为0.72和0.28;当x=0.09时,Mn³⁺离子全部占据16a位置;还得到两种组分16a和24d位置各自的磁矩值。在外磁场(800—10KOe)下测量Y₃Fe_5-xMn_xO₁₂(x=0—0.11)的磁化曲线,温度范围是1.5—300K。得到饱和磁矩值;并利用趋近饱和定律确定1.5K下的磁晶各向异性常数k₁值,发现|k₁|值随含锰量增加而减小。 关键词：     

EPR of Mn2+ doping unannealed single crystal of (La2O3)0.95(CeO2)0.05

X-band room temperature EPR spectra have been recorded for Mn²⁺ ion doping unannealed (La₂O₃)_0.95(CeO₂)_0.05 host crystal. The data are analysed using a rigorous least-squares fitting procedure in which a large number of lines characterized by ΔM = ± 1, Δm = 0 transition, obtained for several orientations of the static magnetic field, are simultaneously fitted. Combined with the knowledge of the absolute sign of the hyperfine interaction parameter. A, the hyperfine Hamiltonian parameters A, B, Q as reported in this paper, are given with their correct signs. The information on the linewidth is used to deduce the deviation of the crystal-field axes of different Mn²⁺ ions from the c axis; on the basis of the model proposed here these deviations are found to be between 0 and 10°.     

Optical absorption spectra and magnetic phase transitions in TbFe<Subscript>3</Subscript>(BO<Subscript>3</Subscript>)<Subscript>4</Subscript>

Optical absorption spectra of the trigonal crystal of TbFe₃(BO₃)₄ in the vicinity of the ⁷F₆ → ⁵D₄ transition in a Tb³⁺ ion were studied as a function of temperature (2–70 K) and magnetic field strength (0–60 kOe) at 2 K. The splitting of the excited states of Tb³⁺ due to both the magnetic ordering of iron and an external magnetic field was determined. Abrupt splitting of the absorption lines of Tb³⁺ at temperature T_N of the magnetic ordering of the subsystem of iron was revealed, suggesting that the nature of such splitting is not entirely magnetic.     

Static and dynamic magnetic characteristics of BaCo0.5Mn0.5Ti1.0Fe10O19

The effect of Mn²⁺Co²⁺Ti⁴⁺ substitution on microwave absorption has been studied for BaCo_0.5Mn_0.5Ti_1.0Fe₁₀O₁₉ ferrite-acrylic resin composites in frequency range from 12 to 20 GHz. X-ray diffraction (XRD), scanning electron microscope (SEM), vibrating sample magnetometer, AC susceptometer and vector network analyzer were used to analyze the structural, magnetic and microwave absorption properties. The results showed that the magnetoplumbite structures for all samples have been formed. Based on microwave measurement on reflectivity, BaCo_0.5Mn_0.5Ti_1.0Fe₁₀O₁₉ may be a good candidate for electromagnetic compatibility and other practical applications at high frequency.