Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Journal of Luminescence

Mixing of the f2(1S0) and 4f5d states of Pr3+ in BaSO4 under high pressure

J.W. Wang, R. Turos-Matysiak, M. Grinberg, William M. Yen, Richard S. Meltzer

Published Mar 1, 2006• 6 citations
Publisher
DOI
10.1016/j.jlumin.2006.01.037

Related papers

4f2 to 4f5d excited state absorption in Pr3+-doped crystals

S Nicolas, E Descroix, Yannick Guyot +5 more

Optical Materials•Feb 1, 2001•29 citations

Excitation of the 1S0 state of Pr3+ in crystal hosts

Christopher G. Levey, Thomas J. Glynn, William M. Yen

Journal of Luminescence•Dec 1, 1984•31 citations

Resonant two-photon cross-section calculations for transitions to 4f5d state in Pr3+:YAG using density matrix theory

Zhenwen Dai, Jingyao Liub, Siyuan Zhang

Physics Letters A•Jan 1, 2000•2 citations

Optical hole burning of Eu3+ and Pr3+ in disordered mixed crystals

K. W. Jang, Kyong-Soo Hong, Tasoltan T. Basiev +1 more

Journal of Luminescence•Dec 1, 1995•3 citations

Excitation of the 1S0 State of Pr3+ in Crystal Hosts

Christopher G. Levey, Thomas J. Glynn, William M. Yen

We excite the (4f2)1s0 state directly through a two photon excited state absorption (from the 1D2 level) and indirectly through excitation of the 4f5d band (using an ArF excimer laser). In Pr3+:LaF3 the 1S0 state lies below the band, and only 1S0 emission is observed. In most hosts examined, it is above the band, and only 4f5d emission is observed. In Pr3+:CaF2 there are sites with each of these properties, and both 1S0 and 4f5d emission are observed, with a relative strength that is concentration dependent.

International Conference on Luminescence - 1984•Jan 1, 1984•0 citations

Experimental and theoretical investigations of the 4ƒ^2→ 4ƒ5d ground-state and excited-state absorption spectra of Pr^3+ in LiYF_4

Mathieu Laroche, J.L. Doualan, Sylvain Girard +2 more

Near-UV excited-state absorption spectra obtained with a pulsed pump–probe technique were recorded in LiYF4:Pr3+ at 77 and at 8 K and revealed a detailed structure of the 4f2 1D2→4f5d and 4f2 (3P0+1I6)→4f5d optical transitions. These experimental results, together with those previously obtained at room temperature, are compared with the numerical predictions of a full calculation of the 4f5d sublevels and of the electric dipole transitions toward these sublevels from different states of the 4f2 configuration. The agreement is good, provided that the four adjustable parameters of the theory are taken as B20(5d)=7290 cm-1,B40(5d)=-14 900 cm-1,F0=60 557 cm-1, and 〈r〉fd=0.245 Å. The level structure of the 4f5d configuration of LiYF4:Pr3+ is shown to be dominated, as expected, by the crystal field coupling of the 5d electron but also, to a noticeable extent, by the spin–orbit coupling of the 4f electron and the Coulomb repulsion of both electrons. The former of these two interactions is somewhat more efficient than the latter in the low-energy part of the 4f5d configuration, i.e., in the spectral region where the largest amount of experimental data is currently available.

Journal of the Optical Society of America B•Jul 1, 2000•52 citations
We excite the (4f2)1s0 state directly through a two photon excited state absorption (from the 1D2 level) and indirectly through excitation of the 4f5d band (using an ArF excimer laser). In Pr3+:LaF3 the 1S0 state lies below the band, and only 1S0 emission is observed. In most hosts examined, it is above the band, and only 4f5d emission is observed. In Pr3+:CaF2 there are sites with each of these properties, and both 1S0 and 4f5d emission are observed, with a relative strength that is concentration dependent.
Near-UV excited-state absorption spectra obtained with a pulsed pump–probe technique were recorded in LiYF4:Pr3+ at 77 and at 8 K and revealed a detailed structure of the 4f2 1D2→4f5d and 4f2 (3P0+1I6)→4f5d optical transitions. These experimental results, together with those previously obtained at room temperature, are compared with the numerical predictions of a full calculation of the 4f5d sublevels and of the electric dipole transitions toward these sublevels from different states of the 4f2 configuration. The agreement is good, provided that the four adjustable parameters of the theory are taken as B20(5d)=7290 cm-1,B40(5d)=-14 900 cm-1,F0=60 557 cm-1, and 〈r〉fd=0.245 Å. The level structure of the 4f5d configuration of LiYF4:Pr3+ is shown to be dominated, as expected, by the crystal field coupling of the 5d electron but also, to a noticeable extent, by the spin–orbit coupling of the 4f electron and the Coulomb repulsion of both electrons. The former of these two interactions is somewhat more efficient than the latter in the low-energy part of the 4f5d configuration, i.e., in the spectral region where the largest amount of experimental data is currently available.