{"title":"掺Nd3+的PbMoO4激光晶体的生长和光谱特性","authors":"Zhiliang Dai, Yexi Huang, Mengxue Wang, Hui Shen and Jiayue Xu","doi":"10.1039/D5CE00137D","DOIUrl":null,"url":null,"abstract":"<p >Lead molybdate (PbMoO<small><sub>4</sub></small>, PMO) crystal is a multifunctional material with diverse applications in acoustic-optics, scintillation and lasers. Herein, transparent 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>-doped PMO crystals were readily grown <em>via</em> the Bridgman method, with dimensions of <em>Φ</em> 25.6 mm × 60 mm. The effective segregation coefficients of Nd<small><sup>3+</sup></small> ions for the 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals were 0.58 and 0.63, respectively. The optical and fluorescence spectra were evaluated in detail, and the spectroscopic properties were determined using the Judd–Ofelt (J–O) theory. For 1 mol% Nd<small><sup>3+</sup></small>:PMO crystals, the absorption cross-section at 804 nm was 13.81 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small>, with an FWHM of 20.3 nm. The absorption cross-section and FWHM at 804 nm were calculated to be 9.29 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> and 14.8 nm for 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals, respectively. Additionally, the emission cross-sections at 1.06 μm were calculated as 12.71 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> and 12.79 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> for 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals, respectively. The fluorescence decay time was moderately decreased from 145.84 μs (1 mol% Nd<small><sup>3+</sup></small>:PMO crystal) to 137.83 μs (2 mol% Nd<small><sup>3+</sup></small>:PMO crystal). Compared with other Nd<small><sup>3+</sup></small> ion-doped laser gain medium, Nd<small><sup>3+</sup></small>:PMO crystals were featured with relatively larger absorption cross-sections and emission cross-sections and longer decay times. This work provides a deeper insight into the design of novel laser crystals in the near infrared region.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 32","pages":" 5431-5440"},"PeriodicalIF":2.6000,"publicationDate":"2025-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Growth and spectroscopic properties of Nd3+-doped PbMoO4 laser crystals\",\"authors\":\"Zhiliang Dai, Yexi Huang, Mengxue Wang, Hui Shen and Jiayue Xu\",\"doi\":\"10.1039/D5CE00137D\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Lead molybdate (PbMoO<small><sub>4</sub></small>, PMO) crystal is a multifunctional material with diverse applications in acoustic-optics, scintillation and lasers. Herein, transparent 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>-doped PMO crystals were readily grown <em>via</em> the Bridgman method, with dimensions of <em>Φ</em> 25.6 mm × 60 mm. The effective segregation coefficients of Nd<small><sup>3+</sup></small> ions for the 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals were 0.58 and 0.63, respectively. The optical and fluorescence spectra were evaluated in detail, and the spectroscopic properties were determined using the Judd–Ofelt (J–O) theory. For 1 mol% Nd<small><sup>3+</sup></small>:PMO crystals, the absorption cross-section at 804 nm was 13.81 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small>, with an FWHM of 20.3 nm. The absorption cross-section and FWHM at 804 nm were calculated to be 9.29 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> and 14.8 nm for 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals, respectively. Additionally, the emission cross-sections at 1.06 μm were calculated as 12.71 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> and 12.79 × 10<small><sup>−20</sup></small> cm<small><sup>2</sup></small> for 1 mol% and 2 mol% Nd<small><sup>3+</sup></small>:PMO crystals, respectively. The fluorescence decay time was moderately decreased from 145.84 μs (1 mol% Nd<small><sup>3+</sup></small>:PMO crystal) to 137.83 μs (2 mol% Nd<small><sup>3+</sup></small>:PMO crystal). Compared with other Nd<small><sup>3+</sup></small> ion-doped laser gain medium, Nd<small><sup>3+</sup></small>:PMO crystals were featured with relatively larger absorption cross-sections and emission cross-sections and longer decay times. This work provides a deeper insight into the design of novel laser crystals in the near infrared region.</p>\",\"PeriodicalId\":70,\"journal\":{\"name\":\"CrystEngComm\",\"volume\":\" 32\",\"pages\":\" 5431-5440\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-07-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"CrystEngComm\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/ce/d5ce00137d\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"CrystEngComm","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/ce/d5ce00137d","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
Growth and spectroscopic properties of Nd3+-doped PbMoO4 laser crystals
Lead molybdate (PbMoO4, PMO) crystal is a multifunctional material with diverse applications in acoustic-optics, scintillation and lasers. Herein, transparent 1 mol% and 2 mol% Nd3+-doped PMO crystals were readily grown via the Bridgman method, with dimensions of Φ 25.6 mm × 60 mm. The effective segregation coefficients of Nd3+ ions for the 1 mol% and 2 mol% Nd3+:PMO crystals were 0.58 and 0.63, respectively. The optical and fluorescence spectra were evaluated in detail, and the spectroscopic properties were determined using the Judd–Ofelt (J–O) theory. For 1 mol% Nd3+:PMO crystals, the absorption cross-section at 804 nm was 13.81 × 10−20 cm2, with an FWHM of 20.3 nm. The absorption cross-section and FWHM at 804 nm were calculated to be 9.29 × 10−20 cm2 and 14.8 nm for 2 mol% Nd3+:PMO crystals, respectively. Additionally, the emission cross-sections at 1.06 μm were calculated as 12.71 × 10−20 cm2 and 12.79 × 10−20 cm2 for 1 mol% and 2 mol% Nd3+:PMO crystals, respectively. The fluorescence decay time was moderately decreased from 145.84 μs (1 mol% Nd3+:PMO crystal) to 137.83 μs (2 mol% Nd3+:PMO crystal). Compared with other Nd3+ ion-doped laser gain medium, Nd3+:PMO crystals were featured with relatively larger absorption cross-sections and emission cross-sections and longer decay times. This work provides a deeper insight into the design of novel laser crystals in the near infrared region.