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Effect of Tb3+ co-doping on the electron population densities of Tm3+ in Ge-As-Ga-S glasses

Identifieur interne : 000F56 ( Pascal/Curation ); précédent : 000F55; suivant : 000F57

Effect of Tb3+ co-doping on the electron population densities of Tm3+ in Ge-As-Ga-S glasses

Auteurs : Yong Beom Shin [Corée du Sud] ; Ji Hyun Kim [Corée du Sud] ; You Song Kim [Corée du Sud] ; Jong Heo [Corée du Sud]

Source :

RBID : Pascal:00-0355014

Descripteurs français

English descriptors

Abstract

The 1.48-μm emission properties and electron population densities of the excited levels were investigated for Ge-As-Ga-S glasses doped with Tm3+ or Tm3+/Tb3+. Electron population inversion between the 3H4 and 3F4 levels in Tm3+ cannot be achieved without Tb3+ addition due to the strong cross-relaxation in Tm3+. Co-doping of Tb3+ resulted in the large decrease in the population density of the Tm3+:3F4 level via the energy transfer of Tm3+:3F4→Tb3+:7F0,1,2. Calculated population densities of the two levels in Tm3+ using the rate equations showed that the population inversion became possible through the addition of Tb3+. © 2000 American Institute of Physics.
pA  
A01 01  1    @0 0021-8979
A02 01      @0 JAPIAU
A03   1    @0 J. appl. phys.
A05       @2 88
A06       @2 5
A08 01  1  ENG  @1 Effect of Tb3+ co-doping on the electron population densities of Tm3+ in Ge-As-Ga-S glasses
A11 01  1    @1 SHIN (Yong Beom)
A11 02  1    @1 KIM (Ji Hyun)
A11 03  1    @1 KIM (You Song)
A11 04  1    @1 HEO (Jong)
A14 01      @1 Photonic Glasses Laboratory, Department of Materials Science and Engineering/School of Environmental Engineering, Pohang University of Science and Technology (POSTECH), Pohang, Korea @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut.
A20       @1 2515-2518
A21       @1 2000-09-01
A23 01      @0 ENG
A43 01      @1 INIST @2 126
A44       @0 8100 @1 © 2000 American Institute of Physics. All rights reserved.
A47 01  1    @0 00-0355014
A60       @1 P
A61       @0 A
A64 01  1    @0 Journal of applied physics
A66 01      @0 USA
C01 01    ENG  @0 The 1.48-μm emission properties and electron population densities of the excited levels were investigated for Ge-As-Ga-S glasses doped with Tm3+ or Tm3+/Tb3+. Electron population inversion between the 3H4 and 3F4 levels in Tm3+ cannot be achieved without Tb3+ addition due to the strong cross-relaxation in Tm3+. Co-doping of Tb3+ resulted in the large decrease in the population density of the Tm3+:3F4 level via the energy transfer of Tm3+:3F4→Tb3+:7F0,1,2. Calculated population densities of the two levels in Tm3+ using the rate equations showed that the population inversion became possible through the addition of Tb3+. © 2000 American Institute of Physics.
C02 01  3    @0 001B70H55H
C02 02  3    @0 001B70A55J
C03 01  3  FRE  @0 7855H @2 PAC @4 INC
C03 02  3  FRE  @0 7155J @2 PAC @4 INC
C03 03  3  FRE  @0 Etude expérimentale
C03 03  3  ENG  @0 Experimental study
C03 04  3  FRE  @0 Inversion population
C03 04  3  ENG  @0 Population inversion
C03 05  3  FRE  @0 Verre germanate
C03 05  3  ENG  @0 Germanate glasses
C03 06  3  FRE  @0 Verre chalcogénure
C03 06  3  ENG  @0 Chalcogenide glasses
C03 07  3  FRE  @0 Gallium composé
C03 07  3  ENG  @0 Gallium compounds
C03 08  3  FRE  @0 Terbium @2 NC
C03 08  3  ENG  @0 Terbium @2 NC
C03 09  3  FRE  @0 Thulium @2 NC
C03 09  3  ENG  @0 Thulium @2 NC
C03 10  3  FRE  @0 Etat impureté
C03 10  3  ENG  @0 Impurity states
C03 11  3  FRE  @0 Fluorescence
C03 11  3  ENG  @0 Fluorescence
C03 12  3  FRE  @0 Spectre absorption impureté
C03 12  3  ENG  @0 Impurity absorption spectra
N21       @1 241
N47 01  1    @0 0034M000408

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Le document en format XML

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<title xml:lang="en" level="a">Effect of Tb
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<div type="abstract" xml:lang="en">The 1.48-μm emission properties and electron population densities of the excited levels were investigated for Ge-As-Ga-S glasses doped with Tm
<sup>3+</sup>
or Tm
<sup>3+</sup>
/Tb
<sup>3+</sup>
. Electron population inversion between the
<sup>3</sup>
H
<sub>4</sub>
and
<sup>3</sup>
F
<sub>4</sub>
levels in Tm
<sup>3+</sup>
cannot be achieved without Tb
<sup>3+</sup>
addition due to the strong cross-relaxation in Tm
<sup>3+</sup>
. Co-doping of Tb
<sup>3+</sup>
resulted in the large decrease in the population density of the Tm
<sup>3+</sup>
:
<sup>3</sup>
F
<sub>4</sub>
level via the energy transfer of Tm
<sup>3+</sup>
:
<sup>3</sup>
F
<sub>4</sub>
→Tb
<sup>3+</sup>
:
<sup>7</sup>
F
<sub>0,1,2</sub>
. Calculated population densities of the two levels in Tm
<sup>3+</sup>
using the rate equations showed that the population inversion became possible through the addition of Tb
<sup>3+</sup>
. © 2000 American Institute of Physics.</div>
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<sup>3+</sup>
or Tm
<sup>3+</sup>
/Tb
<sup>3+</sup>
. Electron population inversion between the
<sup>3</sup>
H
<sub>4</sub>
and
<sup>3</sup>
F
<sub>4</sub>
levels in Tm
<sup>3+</sup>
cannot be achieved without Tb
<sup>3+</sup>
addition due to the strong cross-relaxation in Tm
<sup>3+</sup>
. Co-doping of Tb
<sup>3+</sup>
resulted in the large decrease in the population density of the Tm
<sup>3+</sup>
:
<sup>3</sup>
F
<sub>4</sub>
level via the energy transfer of Tm
<sup>3+</sup>
:
<sup>3</sup>
F
<sub>4</sub>
→Tb
<sup>3+</sup>
:
<sup>7</sup>
F
<sub>0,1,2</sub>
. Calculated population densities of the two levels in Tm
<sup>3+</sup>
using the rate equations showed that the population inversion became possible through the addition of Tb
<sup>3+</sup>
. © 2000 American Institute of Physics.</s0>
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