Spectroscopic study of Er-doped Ga 2 Ge 5 S 13 glass for mid-IR laser applications
We present mid-IR spectroscopic characterization of the low-phonon chalcogenide glass, Ga 2 Ge 5 S 13 (GGS) doped with Er 3+ ions. Under the excitation at ∼800 nm, Er 3+ :GGS exhibited broad mid-IR emission bands centered at ∼2.7, ∼3.5, and ∼4.5 µm at room temperature. The emission lifetime of the 4...
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Veröffentlicht in: | Optical materials express 2022-04, Vol.12 (4), p.1627 |
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creator | Brown, Ei Ei Fleischman, Zackery D. McKay, Jason Hommerich, Uwe Palosz, Witold Trivedi, Sudhir Dubinskii, Mark |
description | We present mid-IR spectroscopic characterization of the low-phonon chalcogenide glass, Ga
2
Ge
5
S
13
(GGS) doped with Er
3+
ions. Under the excitation at ∼800 nm, Er
3+
:GGS exhibited broad mid-IR emission bands centered at ∼2.7, ∼3.5, and ∼4.5 µm at room temperature. The emission lifetime of the
4
I
9/2
level of Er
3+
ions in GGS glass was found to be millisecond-long at room temperature. The measured fluorescence lifetimes were nearly independent of temperature, indicating negligibly small nonradiative decay rate for the
4
I
9/2
state, as can be expected for a low-maximum-phonon energy host. The transition line-strengths, radiative lifetimes, fluorescence branching ratios were calculated by using the Judd-Ofelt method. The peak stimulated emission cross-section of the
4
I
9/2
→
4
I
11/2
transition of Er
3+
ion was determined to be ∼0.10×10
−20
cm
2
at room temperature. |
doi_str_mv | 10.1364/OME.451131 |
format | Article |
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2
Ge
5
S
13
(GGS) doped with Er
3+
ions. Under the excitation at ∼800 nm, Er
3+
:GGS exhibited broad mid-IR emission bands centered at ∼2.7, ∼3.5, and ∼4.5 µm at room temperature. The emission lifetime of the
4
I
9/2
level of Er
3+
ions in GGS glass was found to be millisecond-long at room temperature. The measured fluorescence lifetimes were nearly independent of temperature, indicating negligibly small nonradiative decay rate for the
4
I
9/2
state, as can be expected for a low-maximum-phonon energy host. The transition line-strengths, radiative lifetimes, fluorescence branching ratios were calculated by using the Judd-Ofelt method. The peak stimulated emission cross-section of the
4
I
9/2
→
4
I
11/2
transition of Er
3+
ion was determined to be ∼0.10×10
−20
cm
2
at room temperature.</description><identifier>ISSN: 2159-3930</identifier><identifier>EISSN: 2159-3930</identifier><identifier>DOI: 10.1364/OME.451131</identifier><language>eng</language><ispartof>Optical materials express, 2022-04, Vol.12 (4), p.1627</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c761-2b7af31d45437776ce87f0813cb389a0a06c6ebc1ae1615803b93723f05312db3</citedby><cites>FETCH-LOGICAL-c761-2b7af31d45437776ce87f0813cb389a0a06c6ebc1ae1615803b93723f05312db3</cites><orcidid>0000-0002-4102-1006</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,860,27901,27902</link.rule.ids></links><search><creatorcontrib>Brown, Ei Ei</creatorcontrib><creatorcontrib>Fleischman, Zackery D.</creatorcontrib><creatorcontrib>McKay, Jason</creatorcontrib><creatorcontrib>Hommerich, Uwe</creatorcontrib><creatorcontrib>Palosz, Witold</creatorcontrib><creatorcontrib>Trivedi, Sudhir</creatorcontrib><creatorcontrib>Dubinskii, Mark</creatorcontrib><title>Spectroscopic study of Er-doped Ga 2 Ge 5 S 13 glass for mid-IR laser applications</title><title>Optical materials express</title><description>We present mid-IR spectroscopic characterization of the low-phonon chalcogenide glass, Ga
2
Ge
5
S
13
(GGS) doped with Er
3+
ions. Under the excitation at ∼800 nm, Er
3+
:GGS exhibited broad mid-IR emission bands centered at ∼2.7, ∼3.5, and ∼4.5 µm at room temperature. The emission lifetime of the
4
I
9/2
level of Er
3+
ions in GGS glass was found to be millisecond-long at room temperature. The measured fluorescence lifetimes were nearly independent of temperature, indicating negligibly small nonradiative decay rate for the
4
I
9/2
state, as can be expected for a low-maximum-phonon energy host. The transition line-strengths, radiative lifetimes, fluorescence branching ratios were calculated by using the Judd-Ofelt method. The peak stimulated emission cross-section of the
4
I
9/2
→
4
I
11/2
transition of Er
3+
ion was determined to be ∼0.10×10
−20
cm
2
at room temperature.</description><issn>2159-3930</issn><issn>2159-3930</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNpNkE9Lw0AUxBdRsNRe_ATvLKTu25fdTY5SYixUCm3vYbN_JJKasBsP_fZG6sG5zMxlGH6MPSJfI6n8ef9erXOJSHjDFgJlmVFJ_PZfvmerlD75LKlEIcSCHY6jt1Mckh3GzkKavt0FhgBVzNwwege1AQG1BwlHQIKP3qQEYYhw7ly2PcDcfQQzjn1nzdQNX-mB3QXTJ7_68yU7vVanzVu229fbzcsus1phJlptAqHLZU5aa2V9oQMvkGxLRWm44coq31o0HhXKglNbkhYUuCQUrqUle7rO2vl9ij40Y-zOJl4a5M0vj2bm0Vx50A-WSk94</recordid><startdate>20220401</startdate><enddate>20220401</enddate><creator>Brown, Ei Ei</creator><creator>Fleischman, Zackery D.</creator><creator>McKay, Jason</creator><creator>Hommerich, Uwe</creator><creator>Palosz, Witold</creator><creator>Trivedi, Sudhir</creator><creator>Dubinskii, Mark</creator><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-4102-1006</orcidid></search><sort><creationdate>20220401</creationdate><title>Spectroscopic study of Er-doped Ga 2 Ge 5 S 13 glass for mid-IR laser applications</title><author>Brown, Ei Ei ; Fleischman, Zackery D. ; McKay, Jason ; Hommerich, Uwe ; Palosz, Witold ; Trivedi, Sudhir ; Dubinskii, Mark</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c761-2b7af31d45437776ce87f0813cb389a0a06c6ebc1ae1615803b93723f05312db3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Brown, Ei Ei</creatorcontrib><creatorcontrib>Fleischman, Zackery D.</creatorcontrib><creatorcontrib>McKay, Jason</creatorcontrib><creatorcontrib>Hommerich, Uwe</creatorcontrib><creatorcontrib>Palosz, Witold</creatorcontrib><creatorcontrib>Trivedi, Sudhir</creatorcontrib><creatorcontrib>Dubinskii, Mark</creatorcontrib><collection>CrossRef</collection><jtitle>Optical materials express</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Brown, Ei Ei</au><au>Fleischman, Zackery D.</au><au>McKay, Jason</au><au>Hommerich, Uwe</au><au>Palosz, Witold</au><au>Trivedi, Sudhir</au><au>Dubinskii, Mark</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spectroscopic study of Er-doped Ga 2 Ge 5 S 13 glass for mid-IR laser applications</atitle><jtitle>Optical materials express</jtitle><date>2022-04-01</date><risdate>2022</risdate><volume>12</volume><issue>4</issue><spage>1627</spage><pages>1627-</pages><issn>2159-3930</issn><eissn>2159-3930</eissn><abstract>We present mid-IR spectroscopic characterization of the low-phonon chalcogenide glass, Ga
2
Ge
5
S
13
(GGS) doped with Er
3+
ions. Under the excitation at ∼800 nm, Er
3+
:GGS exhibited broad mid-IR emission bands centered at ∼2.7, ∼3.5, and ∼4.5 µm at room temperature. The emission lifetime of the
4
I
9/2
level of Er
3+
ions in GGS glass was found to be millisecond-long at room temperature. The measured fluorescence lifetimes were nearly independent of temperature, indicating negligibly small nonradiative decay rate for the
4
I
9/2
state, as can be expected for a low-maximum-phonon energy host. The transition line-strengths, radiative lifetimes, fluorescence branching ratios were calculated by using the Judd-Ofelt method. The peak stimulated emission cross-section of the
4
I
9/2
→
4
I
11/2
transition of Er
3+
ion was determined to be ∼0.10×10
−20
cm
2
at room temperature.</abstract><doi>10.1364/OME.451131</doi><orcidid>https://orcid.org/0000-0002-4102-1006</orcidid></addata></record> |
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title | Spectroscopic study of Er-doped Ga 2 Ge 5 S 13 glass for mid-IR laser applications |
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