High‐efficiency infrared‐to‐visible upconversion of Er3+ in BaCl2

Highly efficient infrared‐to‐visible upconversion has been observed in Er3+‐doped BaCl2 phosphors. The composition optimized for maximum green emission was around 25ErCl3 (mol %), which contains 5–15 mol % more active Er3+ ions than those in the conventional Er3+‐doped fluoride phosphors. Pumped by a 0.8 μm laser diode with a power density of ∼3 W/cm2, chloride (25ErCl3‐75BaCl2) shows a very bright green emission with the intensity being two orders of magnitude larger than that of the commercially available IR sensor card on which an optimized fluoride phosphor Y0.8Er0.2F3 is pasted. A 0.97 μm laser diode excitation on the chloride yielded blue (0.49 μm), green (0.55 μm), and red (0.66 μm) fluorescences, visually exhibited as a bright greenish‐white emission. The visible fluorescence excited by 0.8, 0.97, or 1.5 μm laser diodes shows quadratic or cubic dependencies on the excitation power over the entire power range for the chlorides but lower dependences for the fluoride. The differences in the upconvers...

[1]  J. Ohwaki,et al.  New efficient upconversion phosphor BaCl/sub 2/:Er under 1.5 mu m excitation , 1993 .

[2]  J. Ohwaki,et al.  Infrared to Visible Upconversion of Er3+ Doped in a Chloride Matrix , 1992 .

[3]  C. A. Millar,et al.  Upconversion pumped green lasing in erbium doped fluorozirconate fibre , 1991 .

[4]  R. Afzal,et al.  Intensity‐dependent upconversion efficiencies of Er3+ ions in heavy‐metal fluoride glass , 1991 .

[5]  J. Jouart,et al.  Upconversion in Er3+-doped fluorite-type crystals pumped by 1.5 μm tunable diode laser , 1990 .

[6]  R. Macfarlane,et al.  Green infrared‐pumped erbium upconversion laser , 1987 .

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

[8]  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 .

[9]  S. Pollack,et al.  Upconversion‐pumped infrared erbium laser , 1986 .

[10]  G. F. Sá,et al.  1.5 μm high detectivity quantum counter by energy transfers in diode pumped glassceramics , 1985 .

[11]  Y. Mita Detection of 1.5‐μm wavelength laser light emission by infrared‐excitable phosphors , 1981 .

[12]  Y. Ohno,et al.  Efficient infrared‐to‐visible conversion in BaY2F8 : Yb,Er crystal by confinement of excitation energy , 1973 .

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

[14]  H. Kuroda,et al.  Mechanism and Controlling Factors of Infrared-to-Visible Conversion Process in Er3+ and Yb3+-Doped Phosphors , 1972 .

[15]  L. Johnson,et al.  Infrared‐Pumped Visible Laser , 1971 .

[16]  F. W. Ostermayer,et al.  Efficiency of Red, Green, and Blue Infrared‐to‐Visible Conversion Sources , 1971 .

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

[18]  H. Moos,et al.  MULTIPHONON ORBIT-LATTICE RELAXATION OF EXCITED STATES OF RARE-EARTH IONS IN CRYSTALS. , 1968 .

[19]  H. W. Moos,et al.  Rare‐Earth Infrared Lifetimes and Exciton Migration Rates in Trichloride Crystals , 1968 .

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

[21]  K. Eisenthal,et al.  Influence of Resonance Transfer on Luminescence Decay , 1964 .

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

[23]  K. Hirao,et al.  CW room temperature upconversion lasing in Er3+-doped fluoride glass fiber , 1992 .

[24]  Kazuyuki Hirao,et al.  Local structure around rare-earth ions in indium- and lead-based fluoride glasses with high upconversion efficiency , 1992 .

[25]  J. C. Wright Up-conversion and excited state energy transfer in rare-earth doped materials , 1976 .