Spectroscopic properties of Tm3+ ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr
Identifieur interne : 000622 ( Pascal/Curation ); précédent : 000621; suivant : 000623Spectroscopic properties of Tm3+ ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr
Auteurs : YONG GYU CHOI [Corée du Sud] ; JAY HYOK SONG [Corée du Sud]Source :
- Optics communications [ 0030-4018 ] ; 2008.
Descripteurs français
- Pascal (Inist)
- Effet Stark, Luminescence, Traitement matériau, Etude expérimentale, Spectre absorption, Spectre émission, Propriété optique, Matériau dopé, Matériau optique, Addition lanthanide, Chalcogénure, Verre chalcogénure, Métal alcalin halogénure, Ion lanthanide, Lanthanide, Addition thulium, Césium Bromure, Transition niveau énergie, 4270C, 7855Q, 8140T, As Ge S.
English descriptors
- KwdEn :
- Absorption spectra, Alkali metal halides, Cesium Bromides, Chalcogenide glasses, Chalcogenides, Doped materials, Emission spectra, Energy-level transitions, Experimental study, Lanthanide ion, Luminescence, Material processing, Optical materials, Optical properties, Rare earth additions, Rare earths, Stark effect, Thulium additions.
Abstract
We have experimentally confirmed that the absorption and emission properties for intra-4f-configurational transitions of Tm3+ ions doped in Ge-As-S glass, one of representative chalcogenide glasses, are modified dramatically upon the introduction of minute amount of Ga and CsBr, tantamount to a low doping level. This compositional adjustment makes local chemical environments of Tm3+ being rearranged spontaneously without any further thermal treatment applied. The hypersensitive 3H6 ↔3F4 transition, in particular, turns out to reflect the modified chemical environments more significantly than other transitions. Redistribution of the stark levels of 3F4 manifold is mainly responsible for the significant changes in emission spectra for 3H4 → 3F4 and 3F4 → 3H6 transitions. Since the addition of small amount of the group III elements and alkali halides alters only the optical properties of rare-earth ions, while keeping thermal stability of the chalcogenide glass hosts unchanged, our compositional adjustment method would be quite useful for practical applications of rare-earth activated chalcogenide glasses.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Spectroscopic properties of Tm<sup>3+</sup>
ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr</title>
<author><name sortKey="Yong Gyu Choi" sort="Yong Gyu Choi" uniqKey="Yong Gyu Choi" last="Yong Gyu Choi">YONG GYU CHOI</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Materials Science and Engineering, Korea Aerospace University</s1>
<s2>Goyang, Gyeonggi 412-791</s2>
<s3>KOR</s3>
<sZ>1 aut.</sZ>
</inist:fA14>
<country>Corée du Sud</country>
</affiliation>
</author>
<author><name sortKey="Jay Hyok Song" sort="Jay Hyok Song" uniqKey="Jay Hyok Song" last="Jay Hyok Song">JAY HYOK SONG</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Material Laboratory, Corporate R&D Centre, Samsung SDI</s1>
<s2>Yongin, Gyeonggi 446-577</s2>
<s3>KOR</s3>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>Corée du Sud</country>
</affiliation>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Spectroscopic properties of Tm<sup>3+</sup>
ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr</title>
<author><name sortKey="Yong Gyu Choi" sort="Yong Gyu Choi" uniqKey="Yong Gyu Choi" last="Yong Gyu Choi">YONG GYU CHOI</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Materials Science and Engineering, Korea Aerospace University</s1>
<s2>Goyang, Gyeonggi 412-791</s2>
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<sZ>1 aut.</sZ>
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<country>Corée du Sud</country>
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<author><name sortKey="Jay Hyok Song" sort="Jay Hyok Song" uniqKey="Jay Hyok Song" last="Jay Hyok Song">JAY HYOK SONG</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Material Laboratory, Corporate R&D Centre, Samsung SDI</s1>
<s2>Yongin, Gyeonggi 446-577</s2>
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<sZ>2 aut.</sZ>
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<country>Corée du Sud</country>
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<series><title level="j" type="main">Optics communications</title>
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<idno type="ISSN">0030-4018</idno>
<imprint><date when="2008">2008</date>
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<seriesStmt><title level="j" type="main">Optics communications</title>
<title level="j" type="abbreviated">Opt. commun.</title>
<idno type="ISSN">0030-4018</idno>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectra</term>
<term>Alkali metal halides</term>
<term>Cesium Bromides</term>
<term>Chalcogenide glasses</term>
<term>Chalcogenides</term>
<term>Doped materials</term>
<term>Emission spectra</term>
<term>Energy-level transitions</term>
<term>Experimental study</term>
<term>Lanthanide ion</term>
<term>Luminescence</term>
<term>Material processing</term>
<term>Optical materials</term>
<term>Optical properties</term>
<term>Rare earth additions</term>
<term>Rare earths</term>
<term>Stark effect</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Effet Stark</term>
<term>Luminescence</term>
<term>Traitement matériau</term>
<term>Etude expérimentale</term>
<term>Spectre absorption</term>
<term>Spectre émission</term>
<term>Propriété optique</term>
<term>Matériau dopé</term>
<term>Matériau optique</term>
<term>Addition lanthanide</term>
<term>Chalcogénure</term>
<term>Verre chalcogénure</term>
<term>Métal alcalin halogénure</term>
<term>Ion lanthanide</term>
<term>Lanthanide</term>
<term>Addition thulium</term>
<term>Césium Bromure</term>
<term>Transition niveau énergie</term>
<term>4270C</term>
<term>7855Q</term>
<term>8140T</term>
<term>As Ge S</term>
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<front><div type="abstract" xml:lang="en">We have experimentally confirmed that the absorption and emission properties for intra-4f-configurational transitions of Tm<sup>3+</sup>
ions doped in Ge-As-S glass, one of representative chalcogenide glasses, are modified dramatically upon the introduction of minute amount of Ga and CsBr, tantamount to a low doping level. This compositional adjustment makes local chemical environments of Tm<sup>3+</sup>
being rearranged spontaneously without any further thermal treatment applied. The hypersensitive 3H<sub>6</sub>
↔<sup>3</sup>
F<sub>4</sub>
transition, in particular, turns out to reflect the modified chemical environments more significantly than other transitions. Redistribution of the stark levels of 3F<sub>4</sub>
manifold is mainly responsible for the significant changes in emission spectra for <sup>3</sup>
H<sub>4</sub>
→ 3F<sub>4</sub>
and <sup>3</sup>
F<sub>4</sub>
→ 3H<sub>6</sub>
transitions. Since the addition of small amount of the group III elements and alkali halides alters only the optical properties of rare-earth ions, while keeping thermal stability of the chalcogenide glass hosts unchanged, our compositional adjustment method would be quite useful for practical applications of rare-earth activated chalcogenide glasses.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Spectroscopic properties of Tm<sup>3+</sup>
ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr</s1>
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<fA11 i1="01" i2="1"><s1>YONG GYU CHOI</s1>
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<fA11 i1="02" i2="1"><s1>JAY HYOK SONG</s1>
</fA11>
<fA14 i1="01"><s1>Department of Materials Science and Engineering, Korea Aerospace University</s1>
<s2>Goyang, Gyeonggi 412-791</s2>
<s3>KOR</s3>
<sZ>1 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Material Laboratory, Corporate R&D Centre, Samsung SDI</s1>
<s2>Yongin, Gyeonggi 446-577</s2>
<s3>KOR</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA20><s1>4358-4362</s1>
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<fC01 i1="01" l="ENG"><s0>We have experimentally confirmed that the absorption and emission properties for intra-4f-configurational transitions of Tm<sup>3+</sup>
ions doped in Ge-As-S glass, one of representative chalcogenide glasses, are modified dramatically upon the introduction of minute amount of Ga and CsBr, tantamount to a low doping level. This compositional adjustment makes local chemical environments of Tm<sup>3+</sup>
being rearranged spontaneously without any further thermal treatment applied. The hypersensitive 3H<sub>6</sub>
↔<sup>3</sup>
F<sub>4</sub>
transition, in particular, turns out to reflect the modified chemical environments more significantly than other transitions. Redistribution of the stark levels of 3F<sub>4</sub>
manifold is mainly responsible for the significant changes in emission spectra for <sup>3</sup>
H<sub>4</sub>
→ 3F<sub>4</sub>
and <sup>3</sup>
F<sub>4</sub>
→ 3H<sub>6</sub>
transitions. Since the addition of small amount of the group III elements and alkali halides alters only the optical properties of rare-earth ions, while keeping thermal stability of the chalcogenide glass hosts unchanged, our compositional adjustment method would be quite useful for practical applications of rare-earth activated chalcogenide glasses.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B70C</s0>
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<fC02 i1="02" i2="3"><s0>001B70H55Q</s0>
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<fC02 i1="03" i2="3"><s0>001B80A40T</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Effet Stark</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Stark effect</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Luminescence</s0>
<s5>04</s5>
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<fC03 i1="02" i2="3" l="ENG"><s0>Luminescence</s0>
<s5>04</s5>
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<s5>05</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Material processing</s0>
<s5>05</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Tratamiento material</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>30</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Spectre absorption</s0>
<s5>41</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Absorption spectra</s0>
<s5>41</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Spectre émission</s0>
<s5>42</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Emission spectra</s0>
<s5>42</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Propriété optique</s0>
<s5>43</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Optical properties</s0>
<s5>43</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>50</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>50</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Matériau optique</s0>
<s5>57</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Optical materials</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Addition lanthanide</s0>
<s5>58</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Rare earth additions</s0>
<s5>58</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Chalcogénure</s0>
<s2>NA</s2>
<s5>61</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Chalcogenides</s0>
<s2>NA</s2>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Verre chalcogénure</s0>
<s5>62</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Chalcogenide glasses</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Métal alcalin halogénure</s0>
<s5>63</s5>
</fC03>
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<s5>63</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Ion lanthanide</s0>
<s5>64</s5>
</fC03>
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<s5>64</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Lantánido ión</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Lanthanide</s0>
<s2>NC</s2>
<s5>65</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Rare earths</s0>
<s2>NC</s2>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>66</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>66</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Césium Bromure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>67</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Cesium Bromides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>67</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Transition niveau énergie</s0>
<s5>68</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Energy-level transitions</s0>
<s5>68</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>4270C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>7855Q</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>8140T</s0>
<s4>INC</s4>
<s5>85</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>As Ge S</s0>
<s4>INC</s4>
<s5>86</s5>
</fC03>
<fN21><s1>245</s1>
</fN21>
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