Optical spectra and crystal-field levels of [cm(H 2O) 9] 3+ ions with C 3h symmetry in isotypic rare-earth triflate and ethyl sulfate salts

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Authors

  • Patric Lindqvist-Reis
  • Clemens Walther
  • Reinhardt Klenze
  • Norman M. Edelstein

External Research Organisations

  • Karlsruhe Institute of Technology (KIT)
  • Lawrence Berkeley National Laboratory
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Details

Original languageEnglish
Pages (from-to)449-458
Number of pages10
JournalJournal of Physical Chemistry C
Volume113
Issue number1
Publication statusPublished - 8 Dec 2008
Externally publishedYes

Abstract

Fluorescence emission and excitation spectra of [Cm(H 2O) 9] 3+ ions with regular and distorted tricapped trigonal prismatic coordination geometries are reported at temperatures of 293 and 20 K. The Cm 3+ impurities are incorporated into the hexagonal crystal lattices of the isotypic [M(H 2O) 9](CF 3SO 3) 3 (M = La (1), Y (2)), and [Y(H 2O) 9](C 2H 5SO 4) 3 (3) salts, and into the low symmetry [La(H 2O) 9]Cl 3 . 15-crown-5 .H 2O (4) salt. Small but significant structural differences in the MO 9 polyhedra influence the crystal-field levels of the 8Ś 7/2 groundstate and the 67/2 excited-state multiplets. Thus, the total 67/2 splitting is smaller in 1-3 (376-393 cm -1) than in 4 (430 cm -1), which explains the marked blue shifts of the emission spectra of 1-3 to those of 4 and Cm 3+(aq) at 293 K. The transitions between the ground state and the two lowest crystal-field levels of the 67/2 multiplets in 1-3 give rise to narrow fluorescence lines at the emitting level at 20 K, resolving the crystal-field levels of the ground state as sharp and narrowly spaced lines. The total ground-state splittings in 1 (8.0 cm -1), 2 (6.0 cm -1), and 3 (7.5 cm -1) are about three to four times larger than those for Cm +3 in LaCl 3 (2.0 cm -1), but four to six times smaller than those for Cm 3+ in [Y(H 2O) 8]Cl 3 . 15-crown-5 (35 cm -1). Inhomogeneous line broadening prevents resolving the ground multiplet levels in 4. Vibronic side bands associated with the 8Ś 7/2- 67/2 transition are observed in the low temperature emission and excitation spectra. The intensities of these side bands are <1% of the parent electronic transition, the stronger ones being located below ̃400 cm -1 and correspond to various CmO 9 skeletal modes. The luminescence lifetimes in 1-4 are between 63 and 74 μs.

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Optical spectra and crystal-field levels of [cm(H 2O) 9] 3+ ions with C 3h symmetry in isotypic rare-earth triflate and ethyl sulfate salts. / Lindqvist-Reis, Patric; Walther, Clemens; Klenze, Reinhardt et al.
In: Journal of Physical Chemistry C, Vol. 113, No. 1, 08.12.2008, p. 449-458.

Research output: Contribution to journalArticleResearchpeer review

Lindqvist-Reis, Patric ; Walther, Clemens ; Klenze, Reinhardt et al. / Optical spectra and crystal-field levels of [cm(H 2O) 9] 3+ ions with C 3h symmetry in isotypic rare-earth triflate and ethyl sulfate salts. In: Journal of Physical Chemistry C. 2008 ; Vol. 113, No. 1. pp. 449-458.
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title = "Optical spectra and crystal-field levels of [cm(H 2O) 9] 3+ ions with C 3h symmetry in isotypic rare-earth triflate and ethyl sulfate salts",
abstract = "Fluorescence emission and excitation spectra of [Cm(H 2O) 9] 3+ ions with regular and distorted tricapped trigonal prismatic coordination geometries are reported at temperatures of 293 and 20 K. The Cm 3+ impurities are incorporated into the hexagonal crystal lattices of the isotypic [M(H 2O) 9](CF 3SO 3) 3 (M = La (1), Y (2)), and [Y(H 2O) 9](C 2H 5SO 4) 3 (3) salts, and into the low symmetry [La(H 2O) 9]Cl 3 . 15-crown-5 .H 2O (4) salt. Small but significant structural differences in the MO 9 polyhedra influence the crystal-field levels of the 8{\'S} 7/2 groundstate and the 6{\'D} 7/2 excited-state multiplets. Thus, the total 6{\'D} 7/2 splitting is smaller in 1-3 (376-393 cm -1) than in 4 (430 cm -1), which explains the marked blue shifts of the emission spectra of 1-3 to those of 4 and Cm 3+(aq) at 293 K. The transitions between the ground state and the two lowest crystal-field levels of the 6{\'D} 7/2 multiplets in 1-3 give rise to narrow fluorescence lines at the emitting level at 20 K, resolving the crystal-field levels of the ground state as sharp and narrowly spaced lines. The total ground-state splittings in 1 (8.0 cm -1), 2 (6.0 cm -1), and 3 (7.5 cm -1) are about three to four times larger than those for Cm +3 in LaCl 3 (2.0 cm -1), but four to six times smaller than those for Cm 3+ in [Y(H 2O) 8]Cl 3 . 15-crown-5 (35 cm -1). Inhomogeneous line broadening prevents resolving the ground multiplet levels in 4. Vibronic side bands associated with the 8{\'S} 7/2- 6{\'D} 7/2 transition are observed in the low temperature emission and excitation spectra. The intensities of these side bands are <1% of the parent electronic transition, the stronger ones being located below{\~ }400 cm -1 and correspond to various CmO 9 skeletal modes. The luminescence lifetimes in 1-4 are between 63 and 74 μs.",
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TY - JOUR

T1 - Optical spectra and crystal-field levels of [cm(H 2O) 9] 3+ ions with C 3h symmetry in isotypic rare-earth triflate and ethyl sulfate salts

AU - Lindqvist-Reis, Patric

AU - Walther, Clemens

AU - Klenze, Reinhardt

AU - Edelstein, Norman M.

PY - 2008/12/8

Y1 - 2008/12/8

N2 - Fluorescence emission and excitation spectra of [Cm(H 2O) 9] 3+ ions with regular and distorted tricapped trigonal prismatic coordination geometries are reported at temperatures of 293 and 20 K. The Cm 3+ impurities are incorporated into the hexagonal crystal lattices of the isotypic [M(H 2O) 9](CF 3SO 3) 3 (M = La (1), Y (2)), and [Y(H 2O) 9](C 2H 5SO 4) 3 (3) salts, and into the low symmetry [La(H 2O) 9]Cl 3 . 15-crown-5 .H 2O (4) salt. Small but significant structural differences in the MO 9 polyhedra influence the crystal-field levels of the 8Ś 7/2 groundstate and the 6D́ 7/2 excited-state multiplets. Thus, the total 6D́ 7/2 splitting is smaller in 1-3 (376-393 cm -1) than in 4 (430 cm -1), which explains the marked blue shifts of the emission spectra of 1-3 to those of 4 and Cm 3+(aq) at 293 K. The transitions between the ground state and the two lowest crystal-field levels of the 6D́ 7/2 multiplets in 1-3 give rise to narrow fluorescence lines at the emitting level at 20 K, resolving the crystal-field levels of the ground state as sharp and narrowly spaced lines. The total ground-state splittings in 1 (8.0 cm -1), 2 (6.0 cm -1), and 3 (7.5 cm -1) are about three to four times larger than those for Cm +3 in LaCl 3 (2.0 cm -1), but four to six times smaller than those for Cm 3+ in [Y(H 2O) 8]Cl 3 . 15-crown-5 (35 cm -1). Inhomogeneous line broadening prevents resolving the ground multiplet levels in 4. Vibronic side bands associated with the 8Ś 7/2- 6D́ 7/2 transition are observed in the low temperature emission and excitation spectra. The intensities of these side bands are <1% of the parent electronic transition, the stronger ones being located below ̃400 cm -1 and correspond to various CmO 9 skeletal modes. The luminescence lifetimes in 1-4 are between 63 and 74 μs.

AB - Fluorescence emission and excitation spectra of [Cm(H 2O) 9] 3+ ions with regular and distorted tricapped trigonal prismatic coordination geometries are reported at temperatures of 293 and 20 K. The Cm 3+ impurities are incorporated into the hexagonal crystal lattices of the isotypic [M(H 2O) 9](CF 3SO 3) 3 (M = La (1), Y (2)), and [Y(H 2O) 9](C 2H 5SO 4) 3 (3) salts, and into the low symmetry [La(H 2O) 9]Cl 3 . 15-crown-5 .H 2O (4) salt. Small but significant structural differences in the MO 9 polyhedra influence the crystal-field levels of the 8Ś 7/2 groundstate and the 6D́ 7/2 excited-state multiplets. Thus, the total 6D́ 7/2 splitting is smaller in 1-3 (376-393 cm -1) than in 4 (430 cm -1), which explains the marked blue shifts of the emission spectra of 1-3 to those of 4 and Cm 3+(aq) at 293 K. The transitions between the ground state and the two lowest crystal-field levels of the 6D́ 7/2 multiplets in 1-3 give rise to narrow fluorescence lines at the emitting level at 20 K, resolving the crystal-field levels of the ground state as sharp and narrowly spaced lines. The total ground-state splittings in 1 (8.0 cm -1), 2 (6.0 cm -1), and 3 (7.5 cm -1) are about three to four times larger than those for Cm +3 in LaCl 3 (2.0 cm -1), but four to six times smaller than those for Cm 3+ in [Y(H 2O) 8]Cl 3 . 15-crown-5 (35 cm -1). Inhomogeneous line broadening prevents resolving the ground multiplet levels in 4. Vibronic side bands associated with the 8Ś 7/2- 6D́ 7/2 transition are observed in the low temperature emission and excitation spectra. The intensities of these side bands are <1% of the parent electronic transition, the stronger ones being located below ̃400 cm -1 and correspond to various CmO 9 skeletal modes. The luminescence lifetimes in 1-4 are between 63 and 74 μs.

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