Please use this identifier to cite or link to this item:
http://hdl.handle.net/10397/115609
DC Field | Value | Language |
---|---|---|
dc.contributor | Department of Applied Biology and Chemical Technology | - |
dc.creator | Kai, HY | en_US |
dc.creator | Wong, K | en_US |
dc.creator | Tanner, PA | en_US |
dc.date.accessioned | 2025-10-08T01:17:01Z | - |
dc.date.available | 2025-10-08T01:17:01Z | - |
dc.identifier.uri | http://hdl.handle.net/10397/115609 | - |
dc.language.iso | en | en_US |
dc.publisher | Wiley-VCH Verlag GmbH & Co. KGaA | en_US |
dc.rights | © 2025 The Author(s). Advanced Optical Materials published by Wiley-VCH GmbH. This is an open access article under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits use, distribution and reproduction in any medium, provided the original work is properly cited. | en_US |
dc.rights | The following publication H.-Y. Kai, K.-L. Wong, P. A. Tanner, Tunneling in Persistent Luminescence. Adv. Optical Mater. 2025, 13, 2500793 is available at https://doi.org/10.1002/adom.202500793. | en_US |
dc.subject | Afterglow | en_US |
dc.subject | Fading, localized transition | en_US |
dc.subject | Persistent luminescence | en_US |
dc.subject | Thermoluminescence | en_US |
dc.title | Tunneling in persistent luminescence | en_US |
dc.type | Journal/Magazine Article | en_US |
dc.identifier.volume | 13 | en_US |
dc.identifier.issue | 21 | en_US |
dc.identifier.doi | 10.1002/adom.202500793 | en_US |
dcterms.abstract | An overview of some key points in persistent luminescence (PersL) is provided with an emphasis on tunneling phenomena. Notably, key experimental criteria are provided that can substantiate the occurrence of thermal and athermal tunneling and localized transitions. These are elucidated by reference to a Case Study and to some other relevant works. Many experimental studies of PersL have assigned the mechanism to be tunneling on the basis of the linear relationship of PersL decay between intensity, I, and time, t−k, where k is a constant, or I−1 versus t. However, this relation also applies to the case where there is a uniform distribution of trap levels, which may be evident from the breadth of the TL peak. The key measurement for the assignment of below-conduction band processes is the absence of thermal conductivity. | - |
dcterms.accessRights | open access | en_US |
dcterms.bibliographicCitation | Advanced optical materials, 25 July 2025, v. 13, no. 21, 2500793 | en_US |
dcterms.isPartOf | Advanced optical materials | en_US |
dcterms.issued | 2025-07-25 | - |
dc.identifier.scopus | 2-s2.0-105008176484 | - |
dc.identifier.eissn | 2195-1071 | en_US |
dc.identifier.artn | 2500793 | en_US |
dc.description.validate | 202510 bcch | - |
dc.description.oa | Version of Record | en_US |
dc.identifier.FolderNumber | OA_TA | - |
dc.description.fundingSource | RGC | en_US |
dc.description.fundingSource | Others | en_US |
dc.description.fundingText | K.-L.W. acknowledges financial assistance from the Hong Kong Research Grants Council No. 12300021 and NSFC/RGC Joint Research Scheme (N_PolyU209/21). The authors are indebted to Dr. Waygen Thor for reading the manuscript and providing comments. | en_US |
dc.description.pubStatus | Published | en_US |
dc.description.TA | Wiley (2025) | en_US |
dc.description.oaCategory | TA | en_US |
Appears in Collections: | Journal/Magazine Article |
Files in This Item:
File | Description | Size | Format | |
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Kai_Tunneling_Persistent_Luminescence.pdf | 2.58 MB | Adobe PDF | View/Open |
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