Electronic excitations and luminescence of SrMg[F.sub.4] single crystals

The electronic and crystal structures of SrMg[F.sub.4] single crystals grown by the Bridgman method have been investigated. The undoped SrMg[F.sub.4] single crystals have been studied using low-temperature (T = 10 K) time-resolved fluorescence optical and vacuum ultraviolet spectroscopy under select...

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Veröffentlicht in:Physics of the solid state 2014-03, Vol.56 (3), p.456
Hauptverfasser: Pustovarov, V.A, Ogorodnikov, I.N, Omelkov, S.I, Isaenko, L.I, Yelisseyev, A.P, Goloshumova, A.A, Lobanov, S.I, Krinitsyn, P.G
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container_title Physics of the solid state
container_volume 56
creator Pustovarov, V.A
Ogorodnikov, I.N
Omelkov, S.I
Isaenko, L.I
Yelisseyev, A.P
Goloshumova, A.A
Lobanov, S.I
Krinitsyn, P.G
description The electronic and crystal structures of SrMg[F.sub.4] single crystals grown by the Bridgman method have been investigated. The undoped SrMg[F.sub.4] single crystals have been studied using low-temperature (T = 10 K) time-resolved fluorescence optical and vacuum ultraviolet spectroscopy under selective excitation by synchrotron radiation (3.7-36.0 eV). Based on the measured reflectivity spectra and calculated spectra of the optical constants, the following parameters of the electronic structure have been determined for the first time: the minimum energy of interband transitions [E.sub.g] = 12.55 eV, the position of the first exciton peak [E.sub.n = 1] = 11.37 eV, the position of the maximum of the "exciton" luminescence excitation band at 10.7 eV, and the position of the fundamental absorption edge at 10.3 eV. It has been found that photoluminescence excitation occurs predominantly in the region of the low-energy fundamental absorption edge of the crystal and that, at energies above [E.sub.g], the energy transfer from the matrix to luminescence centers is inefficient. The exciton migration is the main excitation channel of photoluminescence bands at 2.6-3.3 and 3.3-4.2 eV. The direct photoexcitation is characteristic of photoluminescence from defects at 1.8-2.6 and 4.2-5.5 eV.
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The undoped SrMg[F.sub.4] single crystals have been studied using low-temperature (T = 10 K) time-resolved fluorescence optical and vacuum ultraviolet spectroscopy under selective excitation by synchrotron radiation (3.7-36.0 eV). Based on the measured reflectivity spectra and calculated spectra of the optical constants, the following parameters of the electronic structure have been determined for the first time: the minimum energy of interband transitions [E.sub.g] = 12.55 eV, the position of the first exciton peak [E.sub.n = 1] = 11.37 eV, the position of the maximum of the "exciton" luminescence excitation band at 10.7 eV, and the position of the fundamental absorption edge at 10.3 eV. It has been found that photoluminescence excitation occurs predominantly in the region of the low-energy fundamental absorption edge of the crystal and that, at energies above [E.sub.g], the energy transfer from the matrix to luminescence centers is inefficient. The exciton migration is the main excitation channel of photoluminescence bands at 2.6-3.3 and 3.3-4.2 eV. 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The exciton migration is the main excitation channel of photoluminescence bands at 2.6-3.3 and 3.3-4.2 eV. 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The exciton migration is the main excitation channel of photoluminescence bands at 2.6-3.3 and 3.3-4.2 eV. The direct photoexcitation is characteristic of photoluminescence from defects at 1.8-2.6 and 4.2-5.5 eV.</abstract><pub>Springer</pub><doi>10.1134/S106378341403024X</doi><tpages>12</tpages></addata></record>
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subjects Crystals
Fluorescence
Nuclear radiation
Photoluminescence
Structure
title Electronic excitations and luminescence of SrMg[F.sub.4] single crystals
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