Inês Proença, José D. Gouveia, Ana V. Girão, Marco Peres, Rodrigo Mateus, Luís C. Alves, Duarte M. Esteves, Ana L. Rodrigues, Maria I. Dias, Katharina Lorenz, Luís Rino, Florinda M. Costa, Teresa Monteiro and Joana Rodrigues
{"title":"Unravelling the UV luminescence of Bi-doped LiYGeO4: a journey from first principles to temperature-dependent photoluminescence","authors":"Inês Proença, José D. Gouveia, Ana V. Girão, Marco Peres, Rodrigo Mateus, Luís C. Alves, Duarte M. Esteves, Ana L. Rodrigues, Maria I. Dias, Katharina Lorenz, Luís Rino, Florinda M. Costa, Teresa Monteiro and Joana Rodrigues","doi":"10.1039/D5TC01676B","DOIUrl":null,"url":null,"abstract":"<p >Materials exhibiting persistent luminescence (PersL) have garnered attention due to their unique ability to emit light for extended periods after the excitation stops. LiYGeO<small><sub>4</sub></small> has arisen as a promising host for PersL due to its notable defect abundance. When doped with Bi, it can provide a long-lasting ultraviolet emission, which may find interesting applications in areas such as photodynamic therapy or self-sustained photocatalysis. In the present paper, undoped and Bi-doped LiYGeO<small><sub>4</sub></small> (0.5 mol%) samples were synthesized by solid-state reaction. X-ray diffraction confirmed the presence of the LiYGeO<small><sub>4</sub></small> phase, alongside residual yttrium germanate phases. Additionally, we calculated its previously undocumented band structure using hybrid density functional theory to provide new theoretical insights. These calculations indicate that LiYGeO<small><sub>4</sub></small> has a direct bandgap at the Γ point, further supported by the absorption data. Elemental analyses allowed quantification of the samples, identifying the loss of Li during the synthesis. Room temperature (RT) photoluminescence (PL) showed a strong emission band peaked around 350–360 nm. Despite the extensive research conducted on LiYGeO<small><sub>4</sub></small>:Bi, the mechanisms underlying the PersL phenomenon remain unclear. To address this, we conducted temperature-dependent PL from 17 K to RT, using a 325 nm photon excitation. We propose that, at RT, the observed emission arises from the overlap of the <small><sup>3</sup></small>P<small><sup>(1)</sup></small><small><sub>1</sub></small> → <small><sup>1</sup></small>S<small><sub>0</sub></small> and <small><sup>3</sup></small>P<small><sup>(2)</sup></small><small><sub>1</sub></small> → <small><sup>1</sup></small>S<small><sub>0</sub></small> Bi<small><sup>3+</sup></small> intraionic transitions, sublevels of the <small><sup>3</sup></small>P<small><sub>1</sub></small> state, which is completely split under the local crystal field generated by the ion environment. However, at cryogenic temperatures, the <small><sup>3</sup></small>P<small><sub>0</sub></small> → <small><sup>1</sup></small>S<small><sub>0</sub></small> transition is the dominant one. Moreover, PersL emission was achieved for nearly 7 h, with 250 nm photon excitation for 10 min, arising from a contribution of the overlapped <small><sup>3</sup></small>P<small><sup>(1)</sup></small><small><sub>1</sub></small> → <small><sup>1</sup></small>S<small><sub>0</sub></small> and <small><sup>3</sup></small>P<small><sup>(2)</sup></small><small><sub>1</sub></small> → <small><sup>1</sup></small>S<small><sub>0</sub></small> transitions.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" 26","pages":" 13167-13183"},"PeriodicalIF":5.1000,"publicationDate":"2025-05-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/tc/d5tc01676b?page=search","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Materials Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/tc/d5tc01676b","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Materials exhibiting persistent luminescence (PersL) have garnered attention due to their unique ability to emit light for extended periods after the excitation stops. LiYGeO4 has arisen as a promising host for PersL due to its notable defect abundance. When doped with Bi, it can provide a long-lasting ultraviolet emission, which may find interesting applications in areas such as photodynamic therapy or self-sustained photocatalysis. In the present paper, undoped and Bi-doped LiYGeO4 (0.5 mol%) samples were synthesized by solid-state reaction. X-ray diffraction confirmed the presence of the LiYGeO4 phase, alongside residual yttrium germanate phases. Additionally, we calculated its previously undocumented band structure using hybrid density functional theory to provide new theoretical insights. These calculations indicate that LiYGeO4 has a direct bandgap at the Γ point, further supported by the absorption data. Elemental analyses allowed quantification of the samples, identifying the loss of Li during the synthesis. Room temperature (RT) photoluminescence (PL) showed a strong emission band peaked around 350–360 nm. Despite the extensive research conducted on LiYGeO4:Bi, the mechanisms underlying the PersL phenomenon remain unclear. To address this, we conducted temperature-dependent PL from 17 K to RT, using a 325 nm photon excitation. We propose that, at RT, the observed emission arises from the overlap of the 3P(1)1 → 1S0 and 3P(2)1 → 1S0 Bi3+ intraionic transitions, sublevels of the 3P1 state, which is completely split under the local crystal field generated by the ion environment. However, at cryogenic temperatures, the 3P0 → 1S0 transition is the dominant one. Moreover, PersL emission was achieved for nearly 7 h, with 250 nm photon excitation for 10 min, arising from a contribution of the overlapped 3P(1)1 → 1S0 and 3P(2)1 → 1S0 transitions.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors