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Bandgap Fluctuations, Hot Carriers, and Band‐to‐Acceptor Recombination in Cu2ZnSn(S,Se)4 Microcrystals
Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S x Se1−x )4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The average depth of these fluctuations is approximately 79 meV. The shape of the corresponding wide photolumi...
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Published in: | Physica status solidi. PSS-RRL. Rapid research letters 2023-09, Vol.17 (9), p.n/a |
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description | Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The average depth of these fluctuations is approximately 79 meV. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The temperature dependence of this PL band is demonstrated to be influenced by the redistribution of holes between potential wells in the valence band with varying depths. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced. This temperature is found to be approximately 300 K higher than the lattice temperature in the samples, and it is mainly caused by the very short minority carrier lifetime. According to the laser power‐dependent PL studies, there is a consistent reduction in the effective carrier temperature as the laser power increases. This phenomenon is explained by the dominance of nonradiative Shockley–Read–Hall recombination at lower temperatures.
Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced. |
doi_str_mv | 10.1002/pssr.202300077 |
format | article |
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x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The average depth of these fluctuations is approximately 79 meV. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The temperature dependence of this PL band is demonstrated to be influenced by the redistribution of holes between potential wells in the valence band with varying depths. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced. This temperature is found to be approximately 300 K higher than the lattice temperature in the samples, and it is mainly caused by the very short minority carrier lifetime. According to the laser power‐dependent PL studies, there is a consistent reduction in the effective carrier temperature as the laser power increases. This phenomenon is explained by the dominance of nonradiative Shockley–Read–Hall recombination at lower temperatures.
Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced.</description><identifier>ISSN: 1862-6254</identifier><identifier>EISSN: 1862-6270</identifier><identifier>DOI: 10.1002/pssr.202300077</identifier><language>eng</language><publisher>Weinheim: Wiley Subscription Services, Inc</publisher><subject>bandgap fluctuations ; Carrier lifetime ; defects ; effective carrier temperature ; Energy gap ; kesterites ; Lasers ; Microcrystals ; Minority carriers ; Photoluminescence ; Temperature ; Temperature dependence ; Valence band</subject><ispartof>Physica status solidi. PSS-RRL. Rapid research letters, 2023-09, Vol.17 (9), p.n/a</ispartof><rights>2023 Wiley‐VCH GmbH</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-8037-5675 ; 0000-0003-0011-1838 ; 0000-0002-1766-4837 ; 0000-0002-4671-2332 ; 0000-0001-6054-6783</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Krustok, Jüri</creatorcontrib><creatorcontrib>Kaupmees, Reelika</creatorcontrib><creatorcontrib>Abbasi, Nafiseh</creatorcontrib><creatorcontrib>Muska, Katri</creatorcontrib><creatorcontrib>Mengü, Idil</creatorcontrib><creatorcontrib>Timmo, Kristi</creatorcontrib><title>Bandgap Fluctuations, Hot Carriers, and Band‐to‐Acceptor Recombination in Cu2ZnSn(S,Se)4 Microcrystals</title><title>Physica status solidi. PSS-RRL. Rapid research letters</title><description>Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The average depth of these fluctuations is approximately 79 meV. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The temperature dependence of this PL band is demonstrated to be influenced by the redistribution of holes between potential wells in the valence band with varying depths. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced. This temperature is found to be approximately 300 K higher than the lattice temperature in the samples, and it is mainly caused by the very short minority carrier lifetime. According to the laser power‐dependent PL studies, there is a consistent reduction in the effective carrier temperature as the laser power increases. This phenomenon is explained by the dominance of nonradiative Shockley–Read–Hall recombination at lower temperatures.
Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced.</description><subject>bandgap fluctuations</subject><subject>Carrier lifetime</subject><subject>defects</subject><subject>effective carrier temperature</subject><subject>Energy gap</subject><subject>kesterites</subject><subject>Lasers</subject><subject>Microcrystals</subject><subject>Minority carriers</subject><subject>Photoluminescence</subject><subject>Temperature</subject><subject>Temperature dependence</subject><subject>Valence band</subject><issn>1862-6254</issn><issn>1862-6270</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNo9kFFLwzAUhYMoOKevPgd8UVjnTdIm7eMszgkTZdUXX0KaptKxNTVpGXvzJ_gb_SV2TvZyzz3w3XvgIHRJYEwA6G3jvRtToAwAhDhCAxJzGnAq4PiwR-EpOvN-CRAlImQDtLxTdfGhGjxddbrtVFvZ2o_wzLY4Vc5VxvWuR_CO-_n6bm0_JlqbprUOL4y267yq_85wVeO0o-91Vl9no8zchPip0s5qt_WtWvlzdFL2Yi7-dYjepvev6SyYPz88ppN50FDGREAIKQmP87hQCeNRqTlNoBAl0XkhDCl4QpK8CKkypYhDzSNKY9CUm5zwIqYhG6Kr_d_G2c_O-FYubefqPlLSmEMoWMKgp5I9talWZisbV62V20oCclem3JUpD2XKlyxbHBz7BQtybGw</recordid><startdate>202309</startdate><enddate>202309</enddate><creator>Krustok, Jüri</creator><creator>Kaupmees, Reelika</creator><creator>Abbasi, Nafiseh</creator><creator>Muska, Katri</creator><creator>Mengü, Idil</creator><creator>Timmo, Kristi</creator><general>Wiley Subscription Services, Inc</general><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-8037-5675</orcidid><orcidid>https://orcid.org/0000-0003-0011-1838</orcidid><orcidid>https://orcid.org/0000-0002-1766-4837</orcidid><orcidid>https://orcid.org/0000-0002-4671-2332</orcidid><orcidid>https://orcid.org/0000-0001-6054-6783</orcidid></search><sort><creationdate>202309</creationdate><title>Bandgap Fluctuations, Hot Carriers, and Band‐to‐Acceptor Recombination in Cu2ZnSn(S,Se)4 Microcrystals</title><author>Krustok, Jüri ; Kaupmees, Reelika ; Abbasi, Nafiseh ; Muska, Katri ; Mengü, Idil ; Timmo, Kristi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p2337-111f168b8da9365fc6290d7f1cbd7e1d6919bd42aef784c652280c26eb16d8243</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>bandgap fluctuations</topic><topic>Carrier lifetime</topic><topic>defects</topic><topic>effective carrier temperature</topic><topic>Energy gap</topic><topic>kesterites</topic><topic>Lasers</topic><topic>Microcrystals</topic><topic>Minority carriers</topic><topic>Photoluminescence</topic><topic>Temperature</topic><topic>Temperature dependence</topic><topic>Valence band</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Krustok, Jüri</creatorcontrib><creatorcontrib>Kaupmees, Reelika</creatorcontrib><creatorcontrib>Abbasi, Nafiseh</creatorcontrib><creatorcontrib>Muska, Katri</creatorcontrib><creatorcontrib>Mengü, Idil</creatorcontrib><creatorcontrib>Timmo, Kristi</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica status solidi. PSS-RRL. Rapid research letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Krustok, Jüri</au><au>Kaupmees, Reelika</au><au>Abbasi, Nafiseh</au><au>Muska, Katri</au><au>Mengü, Idil</au><au>Timmo, Kristi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Bandgap Fluctuations, Hot Carriers, and Band‐to‐Acceptor Recombination in Cu2ZnSn(S,Se)4 Microcrystals</atitle><jtitle>Physica status solidi. PSS-RRL. Rapid research letters</jtitle><date>2023-09</date><risdate>2023</risdate><volume>17</volume><issue>9</issue><epage>n/a</epage><issn>1862-6254</issn><eissn>1862-6270</eissn><abstract>Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The average depth of these fluctuations is approximately 79 meV. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The temperature dependence of this PL band is demonstrated to be influenced by the redistribution of holes between potential wells in the valence band with varying depths. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced. This temperature is found to be approximately 300 K higher than the lattice temperature in the samples, and it is mainly caused by the very short minority carrier lifetime. According to the laser power‐dependent PL studies, there is a consistent reduction in the effective carrier temperature as the laser power increases. This phenomenon is explained by the dominance of nonradiative Shockley–Read–Hall recombination at lower temperatures.
Temperature and laser power dependencies of the band‐to‐acceptor recombination in Cu2ZnSn(S
x
Se1−x
)4 (x = 0.7) microcrystals, which exhibit large bandgap energy fluctuations, are studied. The shape of the corresponding wide photoluminescence (PL) band is analyzed using a modified localized‐state ensemble model. The shape of this band at different temperatures is well fitted when an effective carrier temperature is introduced.</abstract><cop>Weinheim</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/pssr.202300077</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0002-8037-5675</orcidid><orcidid>https://orcid.org/0000-0003-0011-1838</orcidid><orcidid>https://orcid.org/0000-0002-1766-4837</orcidid><orcidid>https://orcid.org/0000-0002-4671-2332</orcidid><orcidid>https://orcid.org/0000-0001-6054-6783</orcidid></addata></record> |
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subjects | bandgap fluctuations Carrier lifetime defects effective carrier temperature Energy gap kesterites Lasers Microcrystals Minority carriers Photoluminescence Temperature Temperature dependence Valence band |
title | Bandgap Fluctuations, Hot Carriers, and Band‐to‐Acceptor Recombination in Cu2ZnSn(S,Se)4 Microcrystals |
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