ThuliumV1, Pascal, Curation, bibRecord, 001198

VUV emission of Er3+ and Tm3 + in fluoride crystals

Identifieur interne : 001198 ( Pascal/Curation ); précédent : 001197; suivant : 001199

VUV emission of Er3+ and Tm3 + in fluoride crystals

Auteurs : J. Becker [Allemagne] ; J. Yu. Gesland [France] ; N. Yu. Kirikova [Russie] ; J. C. Krupa [France] ; V. N. Makhov [Russie] ; M. Runne [Allemagne] ; M. Queffelec [France] ; T. V. Uvarova [Russie] ; G. Zimmerer [Allemagne]

Source :

Journal of luminescence [ 0022-2313 ] ; 1998.

RBID : Pascal:98-0215850

Descripteurs français

Pascal (Inist)
- Etude expérimentale, Addition erbium, Addition thulium, Photoluminescence, Déclin luminescence, Matériau dopé, Transition radiative, Fluorure, 7855F.

English descriptors

KwdEn :
- Doped materials, Erbium additions, Experimental study, Fluorides, Luminescence decay, Photoluminescence, Radiative transition, Thulium additions.

Abstract

VUV emission of several fluoride crystals doped with Er³⁺ and Tm³⁺ has been studied under pulsed synchrotron radiation excitation. It was shown that emission spectra of these ions in the 150-190 nm spectral range consist of both fast emission bands (decay constant in the range from a few to tens of nanoseconds) and slow ones (decay constant in the microsecond range). A model is proposed which explains the co-existence of the slow and fast components by the competition of the parity-allowed interconfiguration 4f^n-15d → 4fⁿ radiative transitions (fast emission) and parity-forbidden intraconfiguration 4fⁿ → 4fⁿ transitions (slow emission). Depending on the relative position of corresponding emitting levels both fast and slow emissions, or only slow, or only fast emission are observed.

A01	`01`	`1`		`@0 0022-2313`
A02	`01`			`@0 JLUMA8`
A03		`1`		`@0 J. lumin.`
A05				`@2 78`
A06				`@2 2`
A08	`01`	`1`	`ENG`	`@1 VUV emission of Er³⁺ and Tm³ ⁺ in fluoride crystals`
A11	`01`	`1`		`@1 BECKER (J.)`
A11	`02`	`1`		`@1 GESLAND (J. Yu.)`
A11	`03`	`1`		`@1 KIRIKOVA (N. Yu.)`
A11	`04`	`1`		`@1 KRUPA (J. C.)`
A11	`05`	`1`		`@1 MAKHOV (V. N.)`
A11	`06`	`1`		`@1 RUNNE (M.)`
A11	`07`	`1`		`@1 QUEFFELEC (M.)`
A11	`08`	`1`		`@1 UVAROVA (T. V.)`
A11	`09`	`1`		`@1 ZIMMERER (G.)`
A14	`01`			`@1 II.Institut fur Experimentalphysik der Universitat Hamburg @2 22761 Hamburg @3 DEU @Z 1 aut. @Z 6 aut. @Z 9 aut.`
A14	`02`			`@1 Universite du Maine @2 Le Mans @3 FRA @Z 2 aut.`
A14	`03`			`@1 Lebedev Physical Institute @2 Moscow 117924 @3 RUS @Z 3 aut. @Z 5 aut.`
A14	`04`			`@1 Institut de Physique Nucleaire @2 91406 Orsay @3 FRA @Z 4 aut. @Z 7 aut.`
A14	`05`			`@1 Institute of General Physics @2 Moscow 117942 @3 RUS @Z 8 aut.`
A20				`@1 91-96`
A21				`@1 1998`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 14666 @5 354000075435730010`
A44				`@0 0000 @1 © 1998 INIST-CNRS. All rights reserved.`
A45				`@0 16 ref.`
A47	`01`	`1`		`@0 98-0215850`
A60				`@1 P`
A61				`@0 A`
A64		`1`		`@0 Journal of luminescence`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 VUV emission of several fluoride crystals doped with Er³⁺ and Tm³⁺ has been studied under pulsed synchrotron radiation excitation. It was shown that emission spectra of these ions in the 150-190 nm spectral range consist of both fast emission bands (decay constant in the range from a few to tens of nanoseconds) and slow ones (decay constant in the microsecond range). A model is proposed which explains the co-existence of the slow and fast components by the competition of the parity-allowed interconfiguration 4f^n-15d → 4fⁿ radiative transitions (fast emission) and parity-forbidden intraconfiguration 4fⁿ → 4fⁿ transitions (slow emission). Depending on the relative position of corresponding emitting levels both fast and slow emissions, or only slow, or only fast emission are observed.
C02	`01`	`3`		`@0 001B70H55F`
C03	`01`	`3`	`FRE`	`@0 Etude expérimentale @5 01`
C03	`01`	`3`	`ENG`	`@0 Experimental study @5 01`
C03	`02`	`3`	`FRE`	`@0 Addition erbium @5 02`
C03	`02`	`3`	`ENG`	`@0 Erbium additions @5 02`
C03	`03`	`3`	`FRE`	`@0 Addition thulium @5 03`
C03	`03`	`3`	`ENG`	`@0 Thulium additions @5 03`
C03	`04`	`3`	`FRE`	`@0 Photoluminescence @5 04`
C03	`04`	`3`	`ENG`	`@0 Photoluminescence @5 04`
C03	`05`	`X`	`FRE`	`@0 Déclin luminescence @5 05`
C03	`05`	`X`	`ENG`	`@0 Luminescence decay @5 05`
C03	`05`	`X`	`SPA`	`@0 Decadencia luminiscencia @5 05`
C03	`06`	`3`	`FRE`	`@0 Matériau dopé @5 06`
C03	`06`	`3`	`ENG`	`@0 Doped materials @5 06`
C03	`07`	`X`	`FRE`	`@0 Transition radiative @5 07`
C03	`07`	`X`	`ENG`	`@0 Radiative transition @5 07`
C03	`07`	`X`	`SPA`	`@0 Transición radiativa @5 07`
C03	`08`	`3`	`FRE`	`@0 Fluorure @2 NA @5 08`
C03	`08`	`3`	`ENG`	`@0 Fluorides @2 NA @5 08`
C03	`09`	`3`	`FRE`	`@0 7855F @2 PAC @4 INC @5 56`
C07	`01`	`3`	`FRE`	`@0 Composé minéral @5 16`
C07	`01`	`3`	`ENG`	`@0 Inorganic compounds @5 16`
N21				`@1 138`

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Pascal:98-0215850

Le document en format XML

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 <sup>+</sup>
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</affiliation>
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<author><name sortKey="Uvarova, T V" sort="Uvarova, T V" uniqKey="Uvarova T" first="T. V." last="Uvarova">T. V. Uvarova</name>
<affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Institute of General Physics</s1>
<s2>Moscow 117942</s2>
<s3>RUS</s3>
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<country>Russie</country>
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<author><name sortKey="Zimmerer, G" sort="Zimmerer, G" uniqKey="Zimmerer G" first="G." last="Zimmerer">G. Zimmerer</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>II.Institut fur Experimentalphysik der Universitat Hamburg</s1>
<s2>22761 Hamburg</s2>
<s3>DEU</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>9 aut.</sZ>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">VUV emission of Er<sup>3+</sup>
 and Tm<sup>3</sup>
 <sup>+</sup>
 in fluoride crystals</title>
<author><name sortKey="Becker, J" sort="Becker, J" uniqKey="Becker J" first="J." last="Becker">J. Becker</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>II.Institut fur Experimentalphysik der Universitat Hamburg</s1>
<s2>22761 Hamburg</s2>
<s3>DEU</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>9 aut.</sZ>
</inist:fA14>
<country>Allemagne</country>
</affiliation>
</author>
<author><name sortKey="Gesland, J Yu" sort="Gesland, J Yu" uniqKey="Gesland J" first="J. Yu." last="Gesland">J. Yu. Gesland</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Universite du Maine</s1>
<s2>Le Mans</s2>
<s3>FRA</s3>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="Kirikova, N Yu" sort="Kirikova, N Yu" uniqKey="Kirikova N" first="N. Yu." last="Kirikova">N. Yu. Kirikova</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Lebedev Physical Institute</s1>
<s2>Moscow 117924</s2>
<s3>RUS</s3>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
</author>
<author><name sortKey="Krupa, J C" sort="Krupa, J C" uniqKey="Krupa J" first="J. C." last="Krupa">J. C. Krupa</name>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Institut de Physique Nucleaire</s1>
<s2>91406 Orsay</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="Makhov, V N" sort="Makhov, V N" uniqKey="Makhov V" first="V. N." last="Makhov">V. N. Makhov</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Lebedev Physical Institute</s1>
<s2>Moscow 117924</s2>
<s3>RUS</s3>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
</author>
<author><name sortKey="Runne, M" sort="Runne, M" uniqKey="Runne M" first="M." last="Runne">M. Runne</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>II.Institut fur Experimentalphysik der Universitat Hamburg</s1>
<s2>22761 Hamburg</s2>
<s3>DEU</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>9 aut.</sZ>
</inist:fA14>
<country>Allemagne</country>
</affiliation>
</author>
<author><name sortKey="Queffelec, M" sort="Queffelec, M" uniqKey="Queffelec M" first="M." last="Queffelec">M. Queffelec</name>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Institut de Physique Nucleaire</s1>
<s2>91406 Orsay</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="Uvarova, T V" sort="Uvarova, T V" uniqKey="Uvarova T" first="T. V." last="Uvarova">T. V. Uvarova</name>
<affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Institute of General Physics</s1>
<s2>Moscow 117942</s2>
<s3>RUS</s3>
<sZ>8 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
</author>
<author><name sortKey="Zimmerer, G" sort="Zimmerer, G" uniqKey="Zimmerer G" first="G." last="Zimmerer">G. Zimmerer</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>II.Institut fur Experimentalphysik der Universitat Hamburg</s1>
<s2>22761 Hamburg</s2>
<s3>DEU</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>9 aut.</sZ>
</inist:fA14>
<country>Allemagne</country>
</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
<imprint><date when="1998">1998</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Doped materials</term>
<term>Erbium additions</term>
<term>Experimental study</term>
<term>Fluorides</term>
<term>Luminescence decay</term>
<term>Photoluminescence</term>
<term>Radiative transition</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude expérimentale</term>
<term>Addition erbium</term>
<term>Addition thulium</term>
<term>Photoluminescence</term>
<term>Déclin luminescence</term>
<term>Matériau dopé</term>
<term>Transition radiative</term>
<term>Fluorure</term>
<term>7855F</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">VUV emission of several fluoride crystals doped with Er<sup>3+</sup>
 and Tm<sup>3+</sup>
 has been studied under pulsed synchrotron radiation excitation. It was shown that emission spectra of these ions in the 150-190 nm spectral range consist of both fast emission bands (decay constant in the range from a few to tens of nanoseconds) and slow ones (decay constant in the microsecond range). A model is proposed which explains the co-existence of the slow and fast components by the competition of the parity-allowed interconfiguration 4f<sup>n-1</sup>
5d → 4f<sup>n</sup>
 radiative transitions (fast emission) and parity-forbidden intraconfiguration 4f<sup>n</sup>
 → 4f<sup>n</sup>
 transitions (slow emission). Depending on the relative position of corresponding emitting levels both fast and slow emissions, or only slow, or only fast emission are observed.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-2313</s0>
</fA01>
<fA02 i1="01"><s0>JLUMA8</s0>
</fA02>
<fA03 i2="1"><s0>J. lumin.</s0>
</fA03>
<fA05><s2>78</s2>
</fA05>
<fA06><s2>2</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>VUV emission of Er<sup>3+</sup>
 and Tm<sup>3</sup>
 <sup>+</sup>
 in fluoride crystals</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>BECKER (J.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>GESLAND (J. Yu.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>KIRIKOVA (N. Yu.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>KRUPA (J. C.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>MAKHOV (V. N.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>RUNNE (M.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>QUEFFELEC (M.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>UVAROVA (T. V.)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>ZIMMERER (G.)</s1>
</fA11>
<fA14 i1="01"><s1>II.Institut fur Experimentalphysik der Universitat Hamburg</s1>
<s2>22761 Hamburg</s2>
<s3>DEU</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Universite du Maine</s1>
<s2>Le Mans</s2>
<s3>FRA</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Lebedev Physical Institute</s1>
<s2>Moscow 117924</s2>
<s3>RUS</s3>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>Institut de Physique Nucleaire</s1>
<s2>91406 Orsay</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="05"><s1>Institute of General Physics</s1>
<s2>Moscow 117942</s2>
<s3>RUS</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA20><s1>91-96</s1>
</fA20>
<fA21><s1>1998</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14666</s2>
<s5>354000075435730010</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 1998 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>16 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>98-0215850</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i2="1"><s0>Journal of luminescence</s0>
</fA64>
<fA66 i1="01"><s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>VUV emission of several fluoride crystals doped with Er<sup>3+</sup>
 and Tm<sup>3+</sup>
 has been studied under pulsed synchrotron radiation excitation. It was shown that emission spectra of these ions in the 150-190 nm spectral range consist of both fast emission bands (decay constant in the range from a few to tens of nanoseconds) and slow ones (decay constant in the microsecond range). A model is proposed which explains the co-existence of the slow and fast components by the competition of the parity-allowed interconfiguration 4f<sup>n-1</sup>
5d → 4f<sup>n</sup>
 radiative transitions (fast emission) and parity-forbidden intraconfiguration 4f<sup>n</sup>
 → 4f<sup>n</sup>
 transitions (slow emission). Depending on the relative position of corresponding emitting levels both fast and slow emissions, or only slow, or only fast emission are observed.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70H55F</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Addition erbium</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Erbium additions</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Photoluminescence</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Photoluminescence</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Déclin luminescence</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Luminescence decay</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Decadencia luminiscencia</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Transition radiative</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Radiative transition</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Transición radiativa</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Fluorure</s0>
<s2>NA</s2>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Fluorides</s0>
<s2>NA</s2>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>7855F</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Composé minéral</s0>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Inorganic compounds</s0>
<s5>16</s5>
</fC07>
<fN21><s1>138</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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VUV emission of Er3+ and Tm3 + in fluoride crystals

VUV emission of Er3+ and Tm3 + in fluoride crystals

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