Selective sensitization of 480-nm blue upconversion by Tm 3+ –Er 3+ energy transfer in tellurite glass

Blue upconversion luminescence at 480 nm resulting from Tm3+:1G4 → 3H6 by 650-nm pumping was selectively sensitized with Er3+ codoped in a tellurite glass. Codoping of Er3+ also quenched the 1D2 → 3F4 luminescence at 450 nm, leading to a single-line blue upconversion. To investigate this sensitized upconversion mechanism, the excitation spectra and the concentration dependence of the lifetimes of the Tm3+ and the Er3+ levels were measured for various doping levels. The Tm3+:3H4 level, which is the intermediate level of excited-state absorption to 1D2, to was found to be depopulated by the energy transfer of Tm3+:3H4 → Er3+:4I9/2 and the Tm3+:3F4 level, which is the intermediate level of excited-state absorption to 1G4, was found to be sensitized by the Er3+:4I13/2 → Tm3+:4F4 energy transfer. The concentration dependence of the transfer rate and of the efficiency of related levels was obtained, and it was concluded that the codoped Er3+ ion is a selective sensitizer in terms of quenching 1D2 upconversion and activating 1G4 upconversion by acting as an acceptor or as a donor for the initial level of each excited-state absorption of the Tm3+ ion.

[1]  D. L. Dexter A Theory of Sensitized Luminescence in Solids , 1953 .

[2]  B. G. Wybourne,et al.  Spectral Intensities of the Trivalent Lanthanides and Actinides in Solution. I. Pr3+, Nd3+, Er3+, Tm3+, and Yb3+ , 1965 .

[3]  Anne C. Tropper,et al.  Frequency upconversion in Tm- and Yb:Tm-doped silica fibers , 1990 .

[4]  Soga,et al.  Compositional dependence of Judd-Ofelt parameters of Er3+ ions in alkali-metal borate glasses. , 1992, Physical review. B, Condensed matter.

[5]  F. Auzel,et al.  Materials and devices using double-pumped-phosphors with energy transfer , 1973 .

[6]  Soga,et al.  Upconversion properties, multiphonon relaxation, and local environment of rare-earth ions in fluorophosphate glasses. , 1992, Physical review. B, Condensed matter.

[7]  M. J. Weber,et al.  Probabilities for Radiative and Nonradiative Decay of Er 3 + in La F 3 , 1967 .

[8]  Jean-Luc Adam,et al.  Optical properties of Tm3+ ions in indium-based fluoride glasses , 1988 .

[9]  William F. Krupke,et al.  Induced-emission cross sections in neodymium laser glasses , 1974 .

[10]  J. P. van der Ziel,et al.  1.5‐μm infrared excitation of visible luminescent in Y1−xErxF3 and Y1−x−yErxTmyF3 via resonant‐energy transfer , 1986 .

[11]  M. J. Suscavage,et al.  Multiphonon relaxation and infrared‐to‐visible conversion of Er3+ and Yb3+ ions in barium‐thorium fluoride glass , 1987 .

[12]  D. L. Dexter,et al.  Phonon Sidebands, Multiphonon Relaxation of Excited States, and Phonon-Assisted Energy Transfer between Ions in Solids , 1970 .

[13]  L. Johnson,et al.  Energy Transfer Between Rare‐Earth Ions , 1966 .

[14]  Setsuhisa Tanabe,et al.  Upconversion fluorescences of TeO2- and Ga2O3-based oxide glasses containing Er3+ , 1990 .

[15]  N. Soga,et al.  Relation between the Ω6 intensity parameter of Er3+ ions and the 151Eu isomer shift in oxide glasses , 1993 .

[16]  Renata Reisfeld,et al.  Eigenstates and radiative transition probabilities for Tm3+ (4f12) in phosphate and tellurite glasses , 1977 .

[17]  B. Judd,et al.  OPTICAL ABSORPTION INTENSITIES OF RARE-EARTH IONS , 1962 .

[18]  G. S. Ofelt Intensities of Crystal Spectra of Rare‐Earth Ions , 1962 .

[19]  N. Soga,et al.  Upconversion and Local Structure of Er3+ Doped Aluminate Glasses , 1993 .

[20]  H. Poignant,et al.  Blue upconversion fluorozirconate fibre laser , 1990 .