Abstract:ESR studies were performed on a single crystal of ferroelectric LiNbO3 doped with manganese. Mn2+ in an axially symmetric site is described by the spin Hamiltonian [H=gβ H·S+B20D20+B40040+B43043+(B43043)*+AS·I]. Values for B43(B43=0, B43I=17 G) reported here, have not been reported previously. By examining the temperature dependence of B43 and B40 a value for the fractional change in the optical parameter Dq[(1/Dq)(∂Dq/∂T)=−3.5 × 10−3 °C−1] has been calculated. A discussion of the temperature dependence of B20… Show more
“…In practice, since D ( = b; = 3B;) is the major parameter which determines the two ZF transitions in (5), Z F splittings can be roughly estimated as 2 0 and 4 0 for 3d5 ions (see, e.g., [28,32,351). …”
Section: Zero-field Splitting Parameters and Energy Levelsmentioning
crystal field (CF) parameters are obtained from the superposition model using two sets of available structural data. Diagonalization of the C F Hamiltonian within the whole 3d5 configuration yields the theoretical Z F splittings. The results for Mn2+ at the Nb site agree better with the experimental data than those for MnZ+ at the Li site. Hence the superposition model analyses of the observed EPR spectra indicate that the spectra can be most likely attributed to Mn'+ ions at Nb sites. The ways to reconcile this conclusion with the opposite one from the low temperature ENDOR study are discussed.
“…In practice, since D ( = b; = 3B;) is the major parameter which determines the two ZF transitions in (5), Z F splittings can be roughly estimated as 2 0 and 4 0 for 3d5 ions (see, e.g., [28,32,351). …”
Section: Zero-field Splitting Parameters and Energy Levelsmentioning
crystal field (CF) parameters are obtained from the superposition model using two sets of available structural data. Diagonalization of the C F Hamiltonian within the whole 3d5 configuration yields the theoretical Z F splittings. The results for Mn2+ at the Nb site agree better with the experimental data than those for MnZ+ at the Li site. Hence the superposition model analyses of the observed EPR spectra indicate that the spectra can be most likely attributed to Mn'+ ions at Nb sites. The ways to reconcile this conclusion with the opposite one from the low temperature ENDOR study are discussed.
“…Another application of solid solutions of LiNbO and LiTaO that contain Eu> is light-converted materials (19)(20)(21)(22)(23)(24). Although some authors have described the optical properties of a single crystal of LiNbO with Mn> (25)(26)(27)(28)(29)(30)(31)(32)(33)(34), no one has reported crystallochemical studies of LiNbO and LiTaO solid solutions with Mn>. Even though our crystallochemical data were in complete agreement with a divalent valence for manganese when it is incorporated into the lattices of LiNbO and the LiTaO , X-ray photoelectron spectroscopy (XPS) was used to confirm this oxidation state, since this technique has proved to be a very powerful tool for the study of molecular bonding (35,36).…”
“…(1) and (2). The D value was already calculated in many previous papers [30][31][32][33]. Only the variation of D values as a function of temperature for Mn 2+ ion is interested in this study.…”
Section: +mentioning
confidence: 99%
“…The local site symmetry, the substituted position and ionic state of the optically active ions in LiNbO 3 crystal can be determined by EPR techniques [28]. A number of NMR [29] and EPR [30][31][32][33] …”
Electron paramagnetic resonance (EPR) spectra of Mn2+ impurity ion in Stoichiometric LiNbO 3 single crystal (SLN) was investigated with an X-band EPR spectrometer in the temperature range of 3 K~296 K. The intensity of EPR spectrum of Mn 2+ ion was increased to 20 K and decreased again below 20 K as the temperature decreases. The zero-field splitting parameter D decreased as the temperature increases. It was suggested that Mn 2+ ion substitute for Nb 5+ ion instead of Li + ion. No changes for hyperfine interaction of Mn
2+ion was obtained in the temperature range of 3 K~296 K.
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