Ion‐pair upconversion pumped laser emission in Er3+ ions in YAG, YLF, SrF2, and CaF2 crystals

Ion‐pair upconversion pumped laser emission at 2.7–2.9 μm between the 4I11/2 and 4I13/2 excited states of triply ionized erbium ions (Er3+) has been studied at 300 and 100 K in YLF, YAG, SrF2, and CaF2 hosts. Laser action was obtained by pumping directly into the transition’s terminal laser level. In all four hosts, the lifetime of the 4I13/2 state is longer than that of the 4I11/2 state, by factors of 5 and 80 for the first two, and factors of (5)/(2) and 2 for the SrF2 and CaF2, respectively. The absorption coefficient for the 1.533‐μm pump radiation is comparable in YLF, SrF2, and CaF2, but is larger by a factor of 3 in YAG. At room temperature the threshold pump energy for YAG is larger by a factor of 10 than for CaF2, SrF2, and YLF. Interpretation of the lasing delay times at threshold pumping levels in terms of a simple analytic model gives for the upconversion coefficients: αYLF =1.2×10−17 cm3 s−1, αYAG =5.4×10−17 cm3 s−1, αSrF2 =2.9×10−15 cm3 s−1, and αCaF2 =3.2×10−15 cm3 s−1. Nonoptimized upconve...

[1]  T. M. Murina,et al.  Cooperative process in Y3Al5O12:Er3+ crystals , 1986 .

[2]  T. M. Murina,et al.  Steady-state emission from a Y3Al5O12:Er3+ laser (λ =2.94 μ, T=300°K) , 1983 .

[3]  G. Dieke,et al.  Ion-Pair Resonance Mechanism of Energy Transfer in Rare Earth Crystal Fluorescence , 1961 .

[4]  N. Bloembergen,et al.  Solid State Infrared Quantum Counters , 1959 .

[5]  S. Pollack,et al.  Upconversion use for viewing and recording infrared images. , 1987, Applied optics.

[6]  A. Prokhorov,et al.  BRIEF COMMUNICATIONS: Erbium-doped CaF2 crystal laser operating at room temperatature , 1975 .

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

[8]  M. Robinson,et al.  THERMAL SWITCHING OF LASER EMISSION OF Er3+ AT 2.69 μ AND Tm3+ AT 1.86 μ IN MIXED CRYSTALS OF CaF2:ErF3:TmF3 , 1967 .

[9]  T. M. Murina,et al.  Cooperative phenomena in yttrium erbium aluminum garnet crystals , 1984 .

[10]  S. Pollack,et al.  Continuous wave and Q‐switched infrared erbium laser , 1986 .

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

[12]  C. Garrett,et al.  Two-Photon Excitation in CaF 2 : Eu 2+ , 1961 .

[13]  T. M. Murina,et al.  Mechanism of a population inversion between the 4I11/2 and 4I13/2 levels of the Er3+ ion in Y3AI5O12 crystals , 1980 .

[14]  T. M. Murina,et al.  Efficient cross-relaxation laser emitting at λ = 2.94 μ , 1983 .

[15]  F. W. Ostermayer,et al.  Infrared‐to‐Visible Conversion by Rare‐Earth Ions in Crystals , 1972 .

[16]  L. Esterowitz,et al.  Rare Earth infrared quantum counter. , 1968, Applied optics.

[17]  T. M. Murina,et al.  Radiative and nonradiative transitions exhibited by Er3+ ions in mixed yttrium-erbium aluminum garnets , 1976 .

[18]  M. I. Timoshechkin,et al.  Stimulated emission from Er3+ ions in yttrium aluminum garnet crystals at λ = 2.94 μ , 1975 .