Abstract:Laser selective excitation and emission spectra as well as σ- and π-polarized absorption spectra have been
recorded for U3+ ions diluted in a CsCdBr3 host crystal. Three distinct U3+ sites were observed. For the
principal site, which was attributed to a symmetric dimer center, 45 crystal-field energy levels in the 0−13250
cm-1 energy range were assigned. These experimentally determined levels were fitted to thirteen parameters
of a semiempirical Hamiltonian representing the combined atomic, one-electron crysta… Show more
“…The consecutive ( i = 1–4) sidebands are coupled to the lines at 20 536 cm –1 (ν i ) and 20 483 cm –1 (ν i ′) of electronic origin and are shifted with respect to these lines by 57 ( i = 1), 99 ( i = 2), 203 ( i = 3), and 256 ( i = 4). The energies of ν 3 and ν 4 vibronic sidebands correspond exactly to those observed also in Ba 2 YCl 7 crystals doped with U 3+ and U 4+ ions …”
Section: Analysis Of Absorption Emission and Excitation
Spectramentioning
confidence: 99%
“…The energies of ν 3 and ν 4 vibronic sidebands correspond exactly to those observed also in Ba 2 YCl 7 crystals doped with U 3+ and U 4+ ions. 20 The combined analysis of the 77 K emission and excitation spectra (Figures 2 and 3) has enabled identification of 66 energy levels for Ba 2 YCl 7 :Pr 3+ , which were subsequently included in the fittings (section 5). Comparison of the experimental and calculated energy levels reveals that only the multiplets 1 G 4 and 1 S 0 have not been experimentally observed, probably due to the equipment limitations.…”
Section: Analysis Of Absorption Emission Andmentioning
Absorption emission and excitation spectra are measured and analyzed to achieve assignments of energy levels for 4f(N) ions in Ba(2)YCl(7):RE(3+) (RE = Pr, Nd, Tb, Dy, Ho, Er, and Tm) crystals. The experimental energy levels were analyzed in terms of the usual free-ion parameters and the crystal field (CF) ones, B(kq), in the Wybourne notation. The orthorhombic C(2v) symmetry is shown to be a good approximation of the actual triclinic C(1) site symmetry at the metal center. The starting values of the CF parameters B(kq) used for fittings for the studied crystals were obtained from superposition model analysis. A good agreement between the calculated and experimental energy levels was obtained with rms deviations in the range from 6.8 cm(-1) (for Ho(3+)) to 14.1 cm(-1) (for Pr(3+)). The fitted sets of B(kq) parameters are, in general, consistent across the 4f(N) series. This study has enabled determination and discussion of the trends in variation of the free-ion parameters and CF ones across the 4f(N) series. The CF parameter set and energy level structure obtained for Nd(3+) ion in Ba(2)YCl(7) crystal are consistent with those for Nd(3+) in structurally related RbY(2)Cl(7) crystal. This systematic analysis of CF parameters is one of only few such studies encompassing nearly whole series of RE(3+) ions.
“…The consecutive ( i = 1–4) sidebands are coupled to the lines at 20 536 cm –1 (ν i ) and 20 483 cm –1 (ν i ′) of electronic origin and are shifted with respect to these lines by 57 ( i = 1), 99 ( i = 2), 203 ( i = 3), and 256 ( i = 4). The energies of ν 3 and ν 4 vibronic sidebands correspond exactly to those observed also in Ba 2 YCl 7 crystals doped with U 3+ and U 4+ ions …”
Section: Analysis Of Absorption Emission and Excitation
Spectramentioning
confidence: 99%
“…The energies of ν 3 and ν 4 vibronic sidebands correspond exactly to those observed also in Ba 2 YCl 7 crystals doped with U 3+ and U 4+ ions. 20 The combined analysis of the 77 K emission and excitation spectra (Figures 2 and 3) has enabled identification of 66 energy levels for Ba 2 YCl 7 :Pr 3+ , which were subsequently included in the fittings (section 5). Comparison of the experimental and calculated energy levels reveals that only the multiplets 1 G 4 and 1 S 0 have not been experimentally observed, probably due to the equipment limitations.…”
Section: Analysis Of Absorption Emission Andmentioning
Absorption emission and excitation spectra are measured and analyzed to achieve assignments of energy levels for 4f(N) ions in Ba(2)YCl(7):RE(3+) (RE = Pr, Nd, Tb, Dy, Ho, Er, and Tm) crystals. The experimental energy levels were analyzed in terms of the usual free-ion parameters and the crystal field (CF) ones, B(kq), in the Wybourne notation. The orthorhombic C(2v) symmetry is shown to be a good approximation of the actual triclinic C(1) site symmetry at the metal center. The starting values of the CF parameters B(kq) used for fittings for the studied crystals were obtained from superposition model analysis. A good agreement between the calculated and experimental energy levels was obtained with rms deviations in the range from 6.8 cm(-1) (for Ho(3+)) to 14.1 cm(-1) (for Pr(3+)). The fitted sets of B(kq) parameters are, in general, consistent across the 4f(N) series. This study has enabled determination and discussion of the trends in variation of the free-ion parameters and CF ones across the 4f(N) series. The CF parameter set and energy level structure obtained for Nd(3+) ion in Ba(2)YCl(7) crystal are consistent with those for Nd(3+) in structurally related RbY(2)Cl(7) crystal. This systematic analysis of CF parameters is one of only few such studies encompassing nearly whole series of RE(3+) ions.
“…In recent years, a number of crystal-field analyses of U 3+ ions in polycrystalline samples and single host crystals have been reported. − Since LaCl 3 (refs and ), LiYF 4 (ref ), and Cs 2 MYX 6 (where M = Li or Na and X = Cl or Br) 9,10 were the only host crystals in which the uranium ions were located at a site symmetry higher than C 2 v , we turned our attention toward high-symmetry hosts. Recently, we have completed an analysis on optical spectra and crystal-field (CF) calculations of U 3+ -doped CsCdBr 3 single crystals . The uranium ions incorporated in this host crystal possess C 3 v site symmetry.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, the results of our spectroscopic investigations on U 3+ -doped Cs 3 Lu 2 Cl 9 and Cs 3 Y 2 I 9 single crystals are presented. Due to a similar surrounding of the U 3+ ions, these host crystals together with those of CsCdBr 3 (ref ) and Cs 2 NaYX 6 (X = Cl or Br) 9,10 are suitable for comparison purposes on the influence of the descending site symmetry on the structure of the crystal-field levels. Besides, with the variation of the environment from chloride to iodide ligands, some trends in the energy level structure of the 5f 3 and 5f 2 6d 1 configuration could be investigated.…”
Low-temperature emission and polarized absorption spectra have been recorded for U(3+) ions diluted in Cs(3)Lu(2)Cl(9) and Cs(3)Y(2)I(9) host crystals. The experimental crystal-field levels were fitted to 13 parameters of a semiempirical Hamiltonian representing the combined atomic, one-electron crystal field (CF) as well as two-particle correlation crystal-field (CCF) operators. The red shift of the first f-d transitions from approximately 14,800 cm(-1) in the spectrum of U(3+):Cs(3)Lu(2)Cl(9) to as low as 11,790 cm(-1) in that of U(3+):Cs(3)Y(2)I(9) has been attributed to an increase in the covalence of the U(3+)-X(-) bonds. Comparison of the differences in the Coulomb repulsion strength between U(3+) and Er(3+) ions in Cs(3)Lu(2)Cl(9) and Cs(3)Y(2)I(9) crystals suggests that the 5f electrons of U(3+) ions are more 3d-like than 4f. The CF splitting of the (2)H(9/2) and (4)F(5/2) multiplets is unexpectedly larger for U(3+):Cs(3)Y(2)I(9) than for U(3+):Cs(3)Lu(2)Cl(9), which may be viewed as a result of the proximity of f-d states. For a correct description of the energy level structure of the (2)H(9/)(2) and (4)F(5/2) multiplets, the inclusion of CCF terms in the parametric Hamiltonian has proved to be essential. The larger f-f transition intensities for U(3+):Cs(3)Y(2)I(9) were also considered to be a consequence of the red shift of the first f-d states. The inadequacy in determination of the minor atomic parameters (other than parameters for Coulomb and spin-orbit interactions) and the insufficient inclusion of the influence of excited configuration in the applied CF Hamiltonian are assumed to be the main deficiencies preventing a better agreement between the experimental and calculated energies of CF levels.
“…This paper paved the way for further studies, though it would be an additional 15 years until such analyses were undertaken [4,5]. Recently [6], we revised and completed this paper and also expanded the investigations on, among others, laser selective excitation and emission spectra of U 3+ ions doped in various host crystals with a very high [7,8] or very low [9,10] site symmetry of the ion, as well as on host crystals doped with two different ions [11]. I would like to emphasize here that from among a very large number of Bill Carnall's papers I have shown the enormous scientific importance and inspiring influence of only two of them.…”
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.