1.5 μm photoluminescence and upconversion photoluminescence in GeGaAsS:Er chalcogenide glass

Author:

Prokop Vit1,Strizik Lukas1,Oswald Jiri2,Vlcek Milan3,Benes Ludvik4,Yannopoulos Spyros N.5,Frumarova Bozena6,Wagner Tomas67

Affiliation:

1. Department of General and Inorganic Chemistry, Faculty of Chemical Technology , University of Pardubice , Studentska 573 , Pardubice 532 10 , Czech Republic , Tel.: +420 466 037 000

2. Institute of Physics of the Czech Academy of Sciences v.v.i. , Cukrovarnicka 10, 162 00 , Prague 6 , Czech Republic

3. Institute of Macromolecular Chemistry of the AS CR, v.v.i. , Heyrovskeho nam. 2, 162 00 , Prague 6 , Czech Republic

4. Joint Laboratory of Solid State Chemistry, Faculty of Chemical Technology , University of Pardubice , Pardubice 532 10 , Czech Republic

5. Foundation for Research and Technology-Hellas, Institute of Chemical Engineering Sciences (FORTH/ICE-HT) , P.O. Box 1414, GR-26504 Patras , Greece

6. Center of Materials and Nanotechnology, Faculty of Chemical Technology , University of Pardubice , nam. Cs. legii 565 , Pardubice 530 02 , Czech Republic

7. Department of General and Inorganic Chemistry, Faculty of Chemical Technology , University of Pardubice , Studentska 573 , Pardubice 532 10 , Czech Republic

Abstract

Abstract The paper reports on ≈1.5 μm Stokes photoluminescence (PL) emission and upconversion photoluminescence (UCPL) emission in the visible and near-infrared spectral region in Er3+-doped Ge25Ga8As2S65 chalcogenide glasses at pumping wavelengths of 980 and 1550 nm. The ≈1.5 μm PL emission spectra are broadened with increasing concentration of Er ions which is discussed in terms of radiation trapping and UCPL dynamics affecting the Er3+: 4 I 13/2 level lifetime. The UCPL emission was observed at ≈530, ≈550, ≈660, ≈810 and ≈990 nm and its overall intensity as well as red-to-green UCPL emission intensity ratio increases with increasing Er concentration. To explore the UCPL dynamics we measured double logarithmic dependency of green (≈550 nm) and red (≈660 nm) UCPL emission versus pump power at pumping wavelength of 975 nm. Moreover, we measured quadrature frequency resolved spectroscopy (QFRS) on green UCPL emission (≈550 nm) using 975 nm pumping wavelength and various excitation powers. The QFRS spectra on green UCPL were analyzed in term of QFRS transfer function for three-level model from which we deduced energy transfer upconversion rate w 11 (s−1) originating from Er3+: 4 I 11/2, 4 I 11/24 F 7/2, 4 I 15/2 transitions.

Publisher

Walter de Gruyter GmbH

Subject

General Chemical Engineering,General Chemistry

Reference60 articles.

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3. R. Fairman, B. Ushkov. Semiconducting Chalcogenide Glass II: Properties of Chalcogenide Glasses, Elsevier Inc., San Diego (2004).

4. T. H. Lee, S. I. Simdyankin, J. Hegedus, J. Heo, S. R. Elliott. Phys. Ref. B81, 104204 (2010).

5. R. Fairman, B. Ushkov. Semiconducting Chalcogenide Glass III: Application of Chalcogenide Glasses, Elsevier Inc., San Diego (2004).

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