Spectral Properties and Thermal Quenching of Mn4+ Luminescence in Silicate Garnet Hosts CaY2MgMAlSi2O12 (M = Al, Ga, Sc)
- Authors: Kirm M.1, Oja M.1, Kozlova J.1, Mändar H.1, Vielhauer S.1, Jansen T.2, Jüstel T.2, Khaidukov N.M.3, Makhov V.N.4
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Affiliations:
- Institute of Physics, University of Tartu
- Münster University of Applied Sciences
- Kurnakov Institute of General and Inorganic Chemistry
- Lebedev Physical Institute
- Issue: Vol 61, No 5 (2019)
- Pages: 853-859
- Section: Optical Properties
- URL: https://ogarev-online.ru/1063-7834/article/view/205558
- DOI: https://doi.org/10.1134/S1063783419050147
- ID: 205558
Cite item
Abstract
Multi-component silicate garnet ceramics CaY2MgMAlSi2O12 comprising different cations M = Al, Ga or Sc in octahedral sites doped with Mn4+ ions have been synthesized and studied as novel red-emitting phosphors aiming at warm white pc-LED applications. All synthesized phosphors exhibit Mn4+ luminescence in rather deep red region, the shortest-wavelength spectrum of Mn4+ luminescence (peak wavelength at 668 nm) being obtained for the host with the largest cation M3+ = Sc3+ in the octahedral site. The effect of increasing the energy of the emitting Mn4+2E level with the size of the host cation in octahedral sites is supposed to be the result of decrease of the covalence of the “Mn4+-ligand” bonding with increase of the interionic Mn4+–O2– distance. All studied phosphors demonstrate rather poor thermal stability of Mn4+ photoluminescence with a thermal quenching temperature T1/2 below 200 K, the lowest value being observed for the host with M = Sc. As expected, the decrease of the energy of the O2––Mn4+ charge-transfer state is observed with the increase of the M3+ cation radius, i.e. with the increase of the O2––Mn4+ interionic distance. The thermal quenching temperature of Mn4+ luminescence in the studied phosphors correlates with the energy of the O2––Mn4+ charge transfer state which is supposed to serve as a quenching state for Mn4+ luminescence.
About the authors
M. Kirm
Institute of Physics, University of Tartu
Email: makhov@sci.lebedev.ru
Estonia, Tartu
M. Oja
Institute of Physics, University of Tartu
Email: makhov@sci.lebedev.ru
Estonia, Tartu
J. Kozlova
Institute of Physics, University of Tartu
Email: makhov@sci.lebedev.ru
Estonia, Tartu
H. Mändar
Institute of Physics, University of Tartu
Email: makhov@sci.lebedev.ru
Estonia, Tartu
S. Vielhauer
Institute of Physics, University of Tartu
Email: makhov@sci.lebedev.ru
Estonia, Tartu
T. Jansen
Münster University of Applied Sciences
Email: makhov@sci.lebedev.ru
Germany, Steinfurt
T. Jüstel
Münster University of Applied Sciences
Email: makhov@sci.lebedev.ru
Germany, Steinfurt
N. M. Khaidukov
Kurnakov Institute of General and Inorganic Chemistry
Email: makhov@sci.lebedev.ru
Russian Federation, Moscow
V. N. Makhov
Lebedev Physical Institute
Author for correspondence.
Email: makhov@sci.lebedev.ru
Russian Federation, Moscow
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