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1.
The results of electron paramagnetic resonance (EPR) studies of Dy3+ ions in lead thiogallate PbGa2S4 single crystals have been presented. It has been shown that the ground state of these ions corresponds to the lowest Stark sublevel Γ6 of the term 6 H 15/2. The spectra are well described by the axially symmetric spin Hamiltonian with the effective spin S = 1/2 with the factors g = 15.06 and g = 2.47. The Dy3+ ions substitute Pb2+ ions in the crystal lattice of PbGa2S4. The observed hyperfine structure has allowed to unambiguously interpret the EPR spectra. The hyperfine interaction constants of two odd isotopes of dysprosium in lead thiogallate single crystals have been found to be A = 675 × 10?4 cm?1 and A = 111 × 10?4 cm?1 for 163Dy and A = 472 × 10?4 cm?1 and A = 77 × 10?4 cm?1 for 161Dy.  相似文献   

2.

Powder samples of hydrothermally grown Cr 3+ -doped Cs 2 NaGaF 6 crystals have been investigated with electron paramagnetic resonance spectroscopy at X - (9.5 v GHz) and Q -band (34 v GHz). Analysis of the spectra clearly demonstrates that there are two distinct Cr 3+ centres in the Cs 2 NaGaF 6 crystal, having nearly identical g factors, but differing largely from the viewpoint of their zero field splitting. By using the 53 Cr hyperfine spectra observed with electron nuclear double resonance spectroscopy, it is deduced that these centres have opposite signs for the zero field splitting. The spectroscopic properties of the Cr 3+ centres in the isostructural Cs 2 NaGaF 6 and Cs 2 NaAlF 6 crystals are compared and discussed.  相似文献   

3.
The results of electron paramagnetic resonance (EPR) studies of Ce3+ impurity ions in single crystals of lead thiogallate PbGa2S4 have been reported. The Ce3+ ions substitute for Pb2+ ions in the crystal lattice of PbGa2S4. A number of paramagnetic cerium centers in lead thiogallate have been observed. The spectra are described by the spin Hamiltonian of rhombic symmetry with the effective spin S = 1/2. The g factors of the main cerium centers have been determined. A large number of paramagnetic centers are due to both nonequivalent positions of lead and local charge compensation under the substitution Ce3+ ?? Pb2+.  相似文献   

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5.
ENDOR measurements on the19F? nuclei in the first four shells of KZnF3 containing Dy3+ ions in the cubic site are reported. The values and signs of the hyperfine and transferred hyperfine interaction parameters are determined. The local deformation of the crystal lattice in the vicinity of the impurity ion is estimated. The theoretical analysis of the THFI parameters for the first coordination shell of the F? ions has been carried out. For the Dy3+ ion the influence of spin polarization of the closed 5s and 5p shells is considered for the first time. Spin polarization is shown to play a significant role in the mechanisms of rare-earth ion-ligand coupling.  相似文献   

6.
We report the observation of the electron paramagnetic resonance spectrum of Dy3+ in Pd single crystals. The observed resonance spectrum contains four main lines, one of which varies strongly with crystal orientation suggesting the ion ground state to be a Γ8 quartet. The weak hyperfine lines due to the isotopes Dy161 and Dy163 have also been observed. The results are discussed in terms of Bleaney's Hamiltonian for a Γ8 quartet.  相似文献   

7.
V K Jain  T M Srinivasan 《Pramana》1978,10(2):155-162
The electron paramagnetic resonance of Mn2+ and Gd3+ doped in Pr2Zn3(NO3)12.24H2O single crystals has been studied at X-band. Mn2+ substitutes for two Zn2+ sites, while Gd3+ substitutes for single type of Pr3+ sites. The spin-Hamiltonian analysis of the EPR spectra is presented at 298 K as well as 77 K.  相似文献   

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10.
In this work, spectroscopic characteristics (oscillator strengths, intensity parameters) of intermanifold f–f transitions of Tm3 +, Ho3+and Dy3+ions in garnet crystals are investigated. It has been found that the intensity change of the hypersensitive intermanifold f–f transitions of rare-earth ions in garnet crystals is determined by the characteristics of their local environment.  相似文献   

11.
A microscopy study of the morphology of the damage produced by TEA-CO2 laser pulses in cubic ZnSe single crystals grown from melt is presented. The observed bulk filamentary damage consists of relatively uniformly distributed elementary damaged zones, located at specific sites where absorbing inclusions could exist. Transmission electron microscopy and laser ion mass spectroscopy investigations revealed the absorbing inclusions to be thin graphite foils, originating from the crucible used for crystal growth.  相似文献   

12.
Single crystals with a ZnS structure are of great practical value, in which connection they are studied in detail by different methods including the spectroscopic. In particular, such crystals activated by ion impurities are investigated in detail by the EPR method. However, the spin-lattice relaxation (SLR) of such systems has hardly been studied. Papers studying the SLR of cubic Mn2+ centers [1] and trigonal Nd3+ and Yb3+ [2] centers in ZnS did only appear recently.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 8, pp. 141–143, August, 1978.The authors are grateful to A. I. Ryskin for providing the single crystals for the investigation and to R. Yu. Abdulsabirov for assistance in performing the experiments.  相似文献   

13.
Room temperature EPR spectra of (NH4)2SO4 doped K2SO4 monocrystals irradiated with x-rays show the presence of NH3 + radicals. The EPR parameters areg ‖=2.0037 andg ⊥ = 2.0068;14NA XX=13.75;A YY=24.5;A ZZ=25.5 gauss;1HA XX=A YY=22 andA ZZ=25 gauss. From the14N and1H coupling constants it has been inferred that at room temperature the planar NH3 + radical undergoes rotation about theC 3 axis which corroborates with the equivalence of the protons, but the radical itself is in an asymmetric crystal field environment. The 77K spectra indicate a considerable reduction in the motion of the radical with the free motion almost completely stopped. Part of Ph.D. work of the second author  相似文献   

14.
Halogen donors (chlorine, bromine and iodine) in cadmium sulfide and zinc selenide single crystals (vapor grown platelets with and without halogen dopants) were determined by thermal neutron activation analysis. This approach proved to be simple, rapid and highly selective. The analyzed impurity contents range from 100 ppb to several ppm. Radionuclides used for identification of chlorine, bromide and iodine were 38Cl (t1/2 ≈ 25 min), 82Br (t1/2 ≈35·1 hr) and 128I (t1/2 ≈ 25 min), respectively; these nuclides were radiochemically isolated and measured by gamma scintillation spectrometry. The levels of the impurities measured by this method were then used to identify new types of donor-acceptor pair line spectra and two-electron transitions accociated with chlorine, bromine or iodine impurities. The results were all in good agreement with the suspected lines, and accordingly well characterized.  相似文献   

15.
The YAlO3: Tm3+ single crystal has been studied on a wide-band EPR spectrometer. The EPR spectra of Tm3+ ions in the frequency range of 90–160 GHz have been detected for the first time. It has been confirmed that thulium ions substitute the position of Y3+ in the crystal lattice. The detected spectra have been described with the use of a spin Hamiltonian with the effective spin S = 1/2. A comparative analysis of the orientation of the magnetic axes of the Tm3+ paramagnetic center with earlier data on other rare-earth ions has been performed.  相似文献   

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Optical birefringence of the spatial dispersion type has been observed in cubic ZnSe crystals.  相似文献   

18.
EPR spectra of deep boron in 4H-SiC and 3C-SiC crystals have been observed and studied. Two sites in 4H-SiC produced deep-boron EPR signals, quasi-cubic k and hexagonal h. In both cases the deep-boron center symmetry is close to axial along the c crystal axis, and the g factor anisotropy is about an order of magnitude larger than that for shallow boron centers. In the 3C-SiC crystal, the deep-boron symmetry is also close to axial along one of the four 〈111〉 directions. The model proposed for the deep boron center with acceptor properties is BSi-v C, where BSi is the boron substituting for silicon, and v C is the carbon vacancy, with the BSi-v C direction coinciding in 4HSiC with the hexagonal axis of the crystal for both k and h positions. In the cubic 3C-SiC crystal, there are four equivalent deep boron centers, which represent BSi-v C pairs with the bond directed along one of the four 〈111〉 crystal directions. Fiz. Tverd. Tela (St. Petersburg) 40, 36–40 (January 1998)  相似文献   

19.
The luminescence of Ca2GeO4: Cr4+ single crystals at wavelengths in the range of 1.3 μm upon excitation with a 1-μ m semiconductor laser is investigated in the temperature range up to 573 K. At T<110 K, the Ca2GeO4: Cr4+ crystals are characterized by the electron paramagnetic resonance, which is attributed to the Cr4+ ions substituted for Ge4+ ions. The components of the g tensor and its principal axes are determined. It is revealed that the Cr4+ impurity centers in calcium germanate affect the crystal symmetry to a lesser degree compared to Cr4+ ions in forsterite. The observed deviation of the temperature dependence of the electron paramagnetic resonance from the Curie law is explained by the transition to the excited state with a low activation energy, as is the case in impurity 3d ions in diamond-like semiconductors. The inference is made that the giant effective degeneracy multiplicity of the excited state is associated with the initiation of soft phonon modes in the crystal upon excitation of the defect.  相似文献   

20.
X-band EPR measurements have been made on single crystals of lead telluride doped with gadolinium in nominal concentrations of 0.04, 0.1, 0.5, and 1.0 atomic %. Fully resolved fine structure appropriate to Gd3+ ions in sites of cubic symmetry was observed in the temperature range from 4.2 K to 300 K. The parameters of the spin Hamiltonian were determined from the spectra by diagonalization of the Hamiltonian matrix and the use of a nonlinear least-squares program. The three parameters are independent of concentration and at 4.2 K have the values g=1.9908 ± 0.0002, b4= ?110.16 ± 0.08 MHz and b6 = +2.40 ± 0.02 MHz respectively. The parameter b4 is temperature dependent; the other parameters are not, to within experimental accuracy. An additional resonance line, possibly analogous to the “cluster” line observed in metallic systems, was seen near g=2.  相似文献   

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