Bound exciton engineering approach for tuning the thermal lensing phenomenon in anatase TiO2: Gd nanosystems

IF 3.8 Q2 CHEMISTRY, PHYSICAL
Oriparambil Sivaraman Nirmal Ghosh , Sethuraman Gayathri , Srinivasa Rao Allam , Alok Sharan , S.B. Sruthil Lal , Modigunta Jeevan Kumar Reddy , A.M. Shanmugharaj , Annamraju Kasi Viswanath
{"title":"Bound exciton engineering approach for tuning the thermal lensing phenomenon in anatase TiO2: Gd nanosystems","authors":"Oriparambil Sivaraman Nirmal Ghosh ,&nbsp;Sethuraman Gayathri ,&nbsp;Srinivasa Rao Allam ,&nbsp;Alok Sharan ,&nbsp;S.B. Sruthil Lal ,&nbsp;Modigunta Jeevan Kumar Reddy ,&nbsp;A.M. Shanmugharaj ,&nbsp;Annamraju Kasi Viswanath","doi":"10.1016/j.chphi.2024.100679","DOIUrl":null,"url":null,"abstract":"<div><p>We report a comprehensive investigation of the third-order nonlinear interaction of femtosecond laser pulses with nanostructured anatase TiO<sub>2</sub> doped with varying concentrations of gadolinium impurities. The samples were synthesized using a facile sol‒gel method. The physicochemical characteristics of the prepared samples were investigated using various analytical techniques, including XRD, SEM, TEM, SAED, UV‒Vis, PL and XPS. The average crystallite sizes of the pristine TiO<sub>2-</sub> and Gd (1, 2, and 3 %)-doped TiO<sub>2</sub> nanoparticles were calculated to be 10.9, 9.2, 10.2 and 8.9 nm, respectively. The W-H plots also revealed average crystallite sizes in the range of 13.9, 16.6, 13.9 and 10.4 for pristine and Gd (1, 2, 3 %)-doped TiO<sub>2</sub> nanoparticles. The lattice strain values for pristine and Gd (1, 2, and 3 %) doped TiO<sub>2</sub> nanoparticles were computed as 0.00203, 0.00667, 0.0036 and 0.00262, respectively, from the W‒H plots. The average crystallite size was calculated to 9.2 nm from the TEM images using ImageJ software. The optical band gap values of pristine TiO<sub>2</sub> and Gd (1, 2, and 3 %)-doped TiO<sub>2</sub> nanoparticles were calculated to be 3.3, 3.23, 3.21 and 3.20 eV from the Kubelka–Munk function plot. The emission peaks of pristine and Gd(1,2,3 %) doped TiO<sub>2</sub> nanoparticles were calculated as 3.2, 3.23, 3.26 and 3.32 eV from the photoluminescence spectra recorded at 330 nm photo excitation. The binding energies of the O1s, Ti2P and Gd4d peaks present in the survey scan of TiO<sub>2</sub> nanoparticles doped with one weight percentage of Gd impurity were 528.79, 531.53, 457.53, 463.25 and 149.6 eV, respectively. The third-order nonlinear characteristics of the TiO<sub>2</sub>:Gd samples were probed using the ultrafast laser Z-scan technique. We observed that the density of bound excitons can be regulated by controlling the dopant concentration. The strong oscillatory interactions between photogenerated bound excitons, which act as dipole oscillators with large oscillating frequencies, were recorded using a single-beam femtosecond Z-scan. The third-order nonlinear susceptibility χ(3) for pristine and Gd(1,2,3 %)-doped TiO<sub>2</sub> nanoparticles were calculated as 7.258 × 10<sup>-18</sup>, 9.4 × 10<sup>-18</sup>, 11 × 10<sup>-18</sup> and 13 × 10<sup>-18</sup> cm<sup>2</sup>/V<sup>2</sup>, respectively. The obtained results suggest that the thermal lensing phenomenon in nanostructured anatase TiO<sub>2</sub> can be generated and effectively controlled using a band gap engineering technique. We determined that the small pump power in nonlinear media with controllable band fluctuations can produce large phase distortions in TiO<sub>2</sub>:Gd nanosystems. Our findings reveal that Gd doping induces controlled modification of the electronic structure of TiO<sub>2</sub>, leading to a tailored energy landscape for exciton formation and binding. These findings provide a novel approach for engineering systems of TiO<sub>2</sub>-based nanostructures for energy-efficient optical-limiting nanophotonic systems and optoelectronic-switching devices.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8000,"publicationDate":"2024-07-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002238/pdfft?md5=a37f00c5d6cb58c275e78d76ad972651&pid=1-s2.0-S2667022424002238-main.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Chemical Physics Impact","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2667022424002238","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0

Abstract

We report a comprehensive investigation of the third-order nonlinear interaction of femtosecond laser pulses with nanostructured anatase TiO2 doped with varying concentrations of gadolinium impurities. The samples were synthesized using a facile sol‒gel method. The physicochemical characteristics of the prepared samples were investigated using various analytical techniques, including XRD, SEM, TEM, SAED, UV‒Vis, PL and XPS. The average crystallite sizes of the pristine TiO2- and Gd (1, 2, and 3 %)-doped TiO2 nanoparticles were calculated to be 10.9, 9.2, 10.2 and 8.9 nm, respectively. The W-H plots also revealed average crystallite sizes in the range of 13.9, 16.6, 13.9 and 10.4 for pristine and Gd (1, 2, 3 %)-doped TiO2 nanoparticles. The lattice strain values for pristine and Gd (1, 2, and 3 %) doped TiO2 nanoparticles were computed as 0.00203, 0.00667, 0.0036 and 0.00262, respectively, from the W‒H plots. The average crystallite size was calculated to 9.2 nm from the TEM images using ImageJ software. The optical band gap values of pristine TiO2 and Gd (1, 2, and 3 %)-doped TiO2 nanoparticles were calculated to be 3.3, 3.23, 3.21 and 3.20 eV from the Kubelka–Munk function plot. The emission peaks of pristine and Gd(1,2,3 %) doped TiO2 nanoparticles were calculated as 3.2, 3.23, 3.26 and 3.32 eV from the photoluminescence spectra recorded at 330 nm photo excitation. The binding energies of the O1s, Ti2P and Gd4d peaks present in the survey scan of TiO2 nanoparticles doped with one weight percentage of Gd impurity were 528.79, 531.53, 457.53, 463.25 and 149.6 eV, respectively. The third-order nonlinear characteristics of the TiO2:Gd samples were probed using the ultrafast laser Z-scan technique. We observed that the density of bound excitons can be regulated by controlling the dopant concentration. The strong oscillatory interactions between photogenerated bound excitons, which act as dipole oscillators with large oscillating frequencies, were recorded using a single-beam femtosecond Z-scan. The third-order nonlinear susceptibility χ(3) for pristine and Gd(1,2,3 %)-doped TiO2 nanoparticles were calculated as 7.258 × 10-18, 9.4 × 10-18, 11 × 10-18 and 13 × 10-18 cm2/V2, respectively. The obtained results suggest that the thermal lensing phenomenon in nanostructured anatase TiO2 can be generated and effectively controlled using a band gap engineering technique. We determined that the small pump power in nonlinear media with controllable band fluctuations can produce large phase distortions in TiO2:Gd nanosystems. Our findings reveal that Gd doping induces controlled modification of the electronic structure of TiO2, leading to a tailored energy landscape for exciton formation and binding. These findings provide a novel approach for engineering systems of TiO2-based nanostructures for energy-efficient optical-limiting nanophotonic systems and optoelectronic-switching devices.

Abstract Image

调整锐钛型二氧化钛热透镜现象的束缚激子工程方法:钆纳米系统
我们报告了飞秒激光脉冲与掺杂不同浓度钆杂质的纳米结构锐钛矿二氧化钛之间三阶非线性相互作用的综合研究。样品采用简便的溶胶-凝胶法合成。利用各种分析技术,包括 XRD、SEM、TEM、SAED、UV-Vis、PL 和 XPS,研究了所制备样品的理化特性。经计算,原始二氧化钛和掺杂钆(1%、2% 和 3%)的二氧化钛纳米粒子的平均晶粒大小分别为 10.9、9.2、10.2 和 8.9 纳米。W-H 图还显示,原始和掺杂钆(1%、2%、3%)的二氧化钛纳米粒子的平均晶粒尺寸范围分别为 13.9、16.6、13.9 和 10.4。根据 W-H 图计算出原始和掺杂钆(1%、2% 和 3%)的二氧化钛纳米粒子的晶格应变值分别为 0.00203、0.00667、0.0036 和 0.00262。利用 ImageJ 软件从 TEM 图像中计算出平均晶粒尺寸为 9.2 nm。根据 Kubelka-Munk 函数图计算出原始 TiO2 和掺杂 Gd(1%、2% 和 3%)的 TiO2 纳米粒子的光带隙值分别为 3.3、3.23、3.21 和 3.20 eV。根据在 330 纳米波长光激发下记录的光致发光光谱,计算出原始和掺杂钆(1,2,3 %)的二氧化钛纳米粒子的发射峰分别为 3.2、3.23、3.26 和 3.32 eV。在掺杂了一个重量百分比的 Gd 杂质的 TiO2 纳米粒子的测量扫描中,O1s、Ti2P 和 Gd4d 峰的结合能分别为 528.79、531.53、457.53、463.25 和 149.6 eV。利用超快激光 Z 扫描技术探测了 TiO2:Gd 样品的三阶非线性特性。我们观察到,束缚激子的密度可以通过控制掺杂剂浓度来调节。利用单束飞秒 Z 扫描技术记录了光生束缚激子之间的强烈振荡相互作用,这些激子就像偶极子振荡器一样,具有很大的振荡频率。计算得出原始和掺杂钆(1,2,3 %)的二氧化钛纳米粒子的三阶非线性感度χ(3) 分别为 7.258 × 10-18、9.4 × 10-18、11 × 10-18 和 13 × 10-18 cm2/V2。这些结果表明,利用带隙工程技术可以产生并有效控制锐钛矿二氧化钛纳米结构中的热透镜现象。我们确定,在具有可控带波动的非线性介质中,小泵功率可在 TiO2:Gd 纳米系统中产生大的相位畸变。我们的研究结果表明,掺杂钆可对二氧化钛的电子结构进行可控修改,从而为激子的形成和结合提供量身定制的能谱。这些发现为基于二氧化钛的纳米结构工程系统提供了一种新方法,可用于高能效光限制纳米光子系统和光电开关器件。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Chemical Physics Impact
Chemical Physics Impact Materials Science-Materials Science (miscellaneous)
CiteScore
2.60
自引率
0.00%
发文量
65
审稿时长
46 days
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信