Article(id=1320097960818487745, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320097951234502959, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20240108, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1706803200000, receivedDateStr=2024-02-02, revisedDate=1709049600000, revisedDateStr=2024-02-28, acceptedDate=null, acceptedDateStr=null, onlineDate=1792665480092, onlineDateStr=2026-10-22, pubDate=1724083200000, pubDateStr=2024-08-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792665480092, onlineIssueDateStr=2026-10-22, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792665480092, creator=13701087609, updateTime=1792665480092, updator=13701087609, issue=Issue{id=1320097951234502959, tenantId=1146029695717560320, journalId=1263187385517883426, year='2024', volume='52', issue='8', pageStart='2453', pageEnd='2754', issueExtLink='null', onlineDate='null', pubDate='1724083200000', pubDateStr='2024-08-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792665477808, creator='13701087609', updateTime=1792666336581, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1320101553256640512, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320097951234502959, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1320101553256640513, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320097951234502959, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=2606, endPage=2614, ext={EN=ArticleExt(id=1320097961019814338, articleId=1320097960818487745, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Optical Properties of Zr4+ Doped CsPbI3 Perovskite Quantum Dots Glass, columnId=1321894711959343516, journalTitle=Journal of the Chinese Ceramic Society, columnName=Special Issue on Foundation and Application of Perovskite Doped Glass—Research Article, runingTitle=null, highlight=null, articleAbstract=
Introduction

In recent years, all-inorganic halide perovskite (CsPbX3, X=Cl, Br, I) quantum dots (QDs) have attracted widespread attention due to their excellent optical and electrical properties. They exhibit high photoluminescence (PL) efficiency, narrow emission bandwidth and tunable emission energy at a wide spectral range. However, the poor stability of CsPbX3 QDs under ambient conditions strongly limit their applications. In this work, CsPbI3 QD-doped borosilicate glasses were prepared by high-temperature melting-quenching followed by heat treatment. ZrO2 is employed as the network modifier, which effectively modifies the local network structure of glass. By optimizing the concentration of ZrO2 and the heat treatment temperature or time, the PL efficiency of the glass can be effectively improved. PL intensity of the QDs glass sample demonstrates high stability, which is almost unchanged after multiple heating and cooling cycles between 293 K and 373 K.

Methods

The CsPbI3 QD-doped glasses were prepared by high-temperature melting-quenching followed by heat treatment. All raw materials with the designed ratios were accurately weighed and mixed in an agate mortar for 20 min. After the raw materials were thoroughly mixed, they were placed in a covered alumina crucible and transferred to a muffle furnace for melting at 1200 ℃ for 20 min. Afterwards, the glass melt was quenched onto a steel plate and pressed into a glass plate. Finally, the precursor glass were heat-treated at different temperatures (520-550 ℃) for 4 h and at 530 ℃ for different times (2-12 h) to precipitate the CsPbI3 QDs.

PL spectra, PL decay curves and thermal stability of glass samples were examined with a FLS 980 fluorescence spectrometer. Optical absorption spectra were recorded by using a UV-3600UV-Vis-NIR spectrometer. X-ray diffraction patterns were recorded by using an X'Pert PRO powder diffractometer. The network structure of glass was analyzed by using a Nicolet 6700 spectrometer and an InVia Reflex Raman spectrometer. The photoluminescence quantum yield (PLQY) was measured with an absolute PLQY measurement system.

Results and discussion

From the XRD results, as the heat treatment time increases, two diffraction peaks at angles (2θ) of 28.5° and 35.5° become stronger in intensity, corresponding to the (200) and (211) planes of CsPbI3 QDs, respectively. With increasing the ZrO2 concentration, the diffraction peak of (200) crystal plane shifts to a larger angle, which is attributed to the replacement of larger Pb2+ ions by smaller Zr4+. Based on FTIR and Raman spectra characterizations, the network structure of glass is mainly composed of [BO4], [SiO4] and [BO3] units. As the ZrO2 concentration increases, the fraction of tetrahedral network structure formed by [BO4] and [SiO4] units in the glass increases, leading to an increase in the fraction of the three-dimensional network structure of the glass, therefore inhibiting the crystallization of CsPbI3 QDs and reducing the size of QDs. This results in the blue shift of the absorption edge and emission peak wavelength. From the emission spectra, with increasing the ZrO2 concentration, the PL intensity of the glass samples first increases and then decreases. Both the absorption edge and emission peak wavelength show a clear redshift with increasing the heat treatment temperature or time, which is mainly attributed to the increased size of QDs. According to the PL decay curves, as the ZrO2 concentration increases, the PL lifetime of glass gradually decreases; as the heat treatment temperature increases, the PL lifetime of glass gradually increases. Finally, after multiple heating and cooling cycles at 293-373 K, there was no significant decrease in the PL intensity of the glass.

Conclusions

The CsPbI3 QD-doped borosilicate glass was prepared successfully by high-temperature melting-quenching followed by heat treatment. X-ray diffraction shows that CsPbI3 QDs are precipitated in the glass. With increasing the ZrO2 concentration, the PL intensity of the glass samples first increases and then decreases, and the highest PLQY reaches 32.6%. In addition, the emission peak wavelength and absorption edge show a blue shift, which is attributed to the increased fraction of tetrahedral network structures formed by [BO4] and [SiO4] units in the glass at higher ZrO2 concentrations. Consequently, the increase in the fraction of the three-dimensional network structures of the glass impedes the movement of Cs+, Pb2+ and I-, inhibiting the crystallization of CsPbI3 QDs. After multiple heating and cooling cycles at 293-373 K, there was no significant decrease in the PL intensity of the glass, indicating that Zr4+ doped CsPbI3 perovskite QDs glass has good thermal stability, which may find applications in display, lighting and other fields.

, authors=Zhousu XU1, Peng WANG1, Yijian YANG1, Guojun ZHENG2, Tao MAN3, Yangming WANG4, Xiaofeng LIU5, Jianrong QIU3, authorsList=Zhousu XU, Peng WANG, Yijian YANG, Guojun ZHENG, Tao MAN, Yangming WANG, Xiaofeng LIU, Jianrong QIU, authorCompany=null, correspAuthors=Xiaofeng LIU, authorNote=

XU Zhousu (1981-), male, Ph.D., Associate Professor. E-mail:

, correspAuthorsNote=
LIU Xiaofeng (1982-), male, Ph.D., Associate Professor. E-mail:
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钙钛矿量子点具有优异的光电性能,有望应用于显示、光伏和光电探测等领域,然而,较差的稳定性限制其应用,将钙钛矿量子点嵌入到玻璃中可以有效地提升其稳定性。采用高温熔融-热处理方法制备了Zr4+掺杂CsPbI3量子点硼硅酸盐玻璃。结果表明:CsPbI3量子点在玻璃内部析出,并且随着ZrO2含量增加,由于较小直径的Zr4+取代了较大直径的Pb2+,(200)晶面的衍射峰向大角度偏移;随着ZrO2含量的增加,发光峰和吸收边均出现蓝移,荧光强度和量子效率先增大后减小,荧光寿命逐渐减小;随着ZrO2含量增加,玻璃中[BO4]和[SiO4]四面体网络结构增加,导致玻璃三维网络结构增加,从而抑制了CsPbI3量子点的析晶。本工作表明所制备的玻璃具有良好的热稳定性,能够应用于显示、照明等领域。

, authors=许周速1, 王鹏1, 杨伊健1, 郑国君2, 满涛3, 王阳明4, 刘小峰5, 邱建荣3, authorsList=许周速, 王鹏, 杨伊健, 郑国君, 满涛, 王阳明, 刘小峰, 邱建荣, authorCompany=null, correspAuthors=刘小峰, authorNote=

许周速(1981—),男,博士,副教授。

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刘小峰(1982—),男,博士,副教授。
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Zr4+掺杂CsPbI3钙钛矿量子点玻璃的光学性能
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许周速 1 , 王鹏 1 , 杨伊健 1 , 郑国君 2 , 满涛 3 , 王阳明 4 , 刘小峰 5 , 邱建荣 3
硅酸盐学报 | 钙钛矿掺杂玻璃的基础和应用专题—研究论文 2024,52(8): 2606-2614
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硅酸盐学报 |钙钛矿掺杂玻璃的基础和应用专题—研究论文 2024 , 52 (8) : 2606 -2614
Zr4+掺杂CsPbI3钙钛矿量子点玻璃的光学性能
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许周速1 , 王鹏1, 杨伊健1, 郑国君2, 满涛3, 王阳明4, 刘小峰5 , 邱建荣3
作者信息
  • 1.浙江工业大学光电子智能化技术研究所,杭州 310023
  • 2.宁波大学信息科学与工程学院,浙江 宁波 315211
  • 3.浙江大学光电科学与工程学院,杭州 310027
  • 4.浙江工业大学计算机科学与技术学院,杭州 310023
  • 5.浙江大学材料科学与工程学院,杭州 310027
通讯作者:
刘小峰(1982—),男,博士,副教授。
作者简介:

许周速(1981—),男,博士,副教授。

Optical Properties of Zr4+ Doped CsPbI3 Perovskite Quantum Dots Glass
Zhousu XU1 , Peng WANG1, Yijian YANG1, Guojun ZHENG2, Tao MAN3, Yangming WANG4, Xiaofeng LIU5 , Jianrong QIU3
Affiliations
  • 1.Institute of Intelligent Optoelectronic Technology, Zhejiang University of Technology, Hangzhou 310023, China
  • 2.College of Electrical Engineering and Computer Sciences, Ningbo University, Ningbo 315211, Zhejiang, China
  • 3.College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
  • 4.College of Computer Science and Technology, Zhejiang University of Technology, Hangzhou 310023, China
  • 5.School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
  • Corresponding Author:
    LIU Xiaofeng (1982-), male, Ph.D., Associate Professor. E-mail:

    XU Zhousu (1981-), male, Ph.D., Associate Professor. E-mail:

出版时间: 2024-08-20 doi: 10.14062/j.issn.0454-5648.20240108
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钙钛矿量子点具有优异的光电性能,有望应用于显示、光伏和光电探测等领域,然而,较差的稳定性限制其应用,将钙钛矿量子点嵌入到玻璃中可以有效地提升其稳定性。采用高温熔融-热处理方法制备了Zr4+掺杂CsPbI3量子点硼硅酸盐玻璃。结果表明:CsPbI3量子点在玻璃内部析出,并且随着ZrO2含量增加,由于较小直径的Zr4+取代了较大直径的Pb2+,(200)晶面的衍射峰向大角度偏移;随着ZrO2含量的增加,发光峰和吸收边均出现蓝移,荧光强度和量子效率先增大后减小,荧光寿命逐渐减小;随着ZrO2含量增加,玻璃中[BO4]和[SiO4]四面体网络结构增加,导致玻璃三维网络结构增加,从而抑制了CsPbI3量子点的析晶。本工作表明所制备的玻璃具有良好的热稳定性,能够应用于显示、照明等领域。

锆离子  /  量子点  /  硼硅酸盐玻璃  /  析晶
Introduction

In recent years, all-inorganic halide perovskite (CsPbX3, X=Cl, Br, I) quantum dots (QDs) have attracted widespread attention due to their excellent optical and electrical properties. They exhibit high photoluminescence (PL) efficiency, narrow emission bandwidth and tunable emission energy at a wide spectral range. However, the poor stability of CsPbX3 QDs under ambient conditions strongly limit their applications. In this work, CsPbI3 QD-doped borosilicate glasses were prepared by high-temperature melting-quenching followed by heat treatment. ZrO2 is employed as the network modifier, which effectively modifies the local network structure of glass. By optimizing the concentration of ZrO2 and the heat treatment temperature or time, the PL efficiency of the glass can be effectively improved. PL intensity of the QDs glass sample demonstrates high stability, which is almost unchanged after multiple heating and cooling cycles between 293 K and 373 K.

Methods

The CsPbI3 QD-doped glasses were prepared by high-temperature melting-quenching followed by heat treatment. All raw materials with the designed ratios were accurately weighed and mixed in an agate mortar for 20 min. After the raw materials were thoroughly mixed, they were placed in a covered alumina crucible and transferred to a muffle furnace for melting at 1200 ℃ for 20 min. Afterwards, the glass melt was quenched onto a steel plate and pressed into a glass plate. Finally, the precursor glass were heat-treated at different temperatures (520-550 ℃) for 4 h and at 530 ℃ for different times (2-12 h) to precipitate the CsPbI3 QDs.

PL spectra, PL decay curves and thermal stability of glass samples were examined with a FLS 980 fluorescence spectrometer. Optical absorption spectra were recorded by using a UV-3600UV-Vis-NIR spectrometer. X-ray diffraction patterns were recorded by using an X'Pert PRO powder diffractometer. The network structure of glass was analyzed by using a Nicolet 6700 spectrometer and an InVia Reflex Raman spectrometer. The photoluminescence quantum yield (PLQY) was measured with an absolute PLQY measurement system.

Results and discussion

From the XRD results, as the heat treatment time increases, two diffraction peaks at angles (2θ) of 28.5° and 35.5° become stronger in intensity, corresponding to the (200) and (211) planes of CsPbI3 QDs, respectively. With increasing the ZrO2 concentration, the diffraction peak of (200) crystal plane shifts to a larger angle, which is attributed to the replacement of larger Pb2+ ions by smaller Zr4+. Based on FTIR and Raman spectra characterizations, the network structure of glass is mainly composed of [BO4], [SiO4] and [BO3] units. As the ZrO2 concentration increases, the fraction of tetrahedral network structure formed by [BO4] and [SiO4] units in the glass increases, leading to an increase in the fraction of the three-dimensional network structure of the glass, therefore inhibiting the crystallization of CsPbI3 QDs and reducing the size of QDs. This results in the blue shift of the absorption edge and emission peak wavelength. From the emission spectra, with increasing the ZrO2 concentration, the PL intensity of the glass samples first increases and then decreases. Both the absorption edge and emission peak wavelength show a clear redshift with increasing the heat treatment temperature or time, which is mainly attributed to the increased size of QDs. According to the PL decay curves, as the ZrO2 concentration increases, the PL lifetime of glass gradually decreases; as the heat treatment temperature increases, the PL lifetime of glass gradually increases. Finally, after multiple heating and cooling cycles at 293-373 K, there was no significant decrease in the PL intensity of the glass.

Conclusions

The CsPbI3 QD-doped borosilicate glass was prepared successfully by high-temperature melting-quenching followed by heat treatment. X-ray diffraction shows that CsPbI3 QDs are precipitated in the glass. With increasing the ZrO2 concentration, the PL intensity of the glass samples first increases and then decreases, and the highest PLQY reaches 32.6%. In addition, the emission peak wavelength and absorption edge show a blue shift, which is attributed to the increased fraction of tetrahedral network structures formed by [BO4] and [SiO4] units in the glass at higher ZrO2 concentrations. Consequently, the increase in the fraction of the three-dimensional network structures of the glass impedes the movement of Cs+, Pb2+ and I-, inhibiting the crystallization of CsPbI3 QDs. After multiple heating and cooling cycles at 293-373 K, there was no significant decrease in the PL intensity of the glass, indicating that Zr4+ doped CsPbI3 perovskite QDs glass has good thermal stability, which may find applications in display, lighting and other fields.

zirconium ions  /  quantum dots  /  borosilicate glass  /  crystallization
许周速, 王鹏, 杨伊健, 郑国君, 满涛, 王阳明, 刘小峰, 邱建荣. Zr4+掺杂CsPbI3钙钛矿量子点玻璃的光学性能. 硅酸盐学报, 2024 , 52 (8) : 2606 -2614 . DOI: 10.14062/j.issn.0454-5648.20240108
Zhousu XU, Peng WANG, Yijian YANG, Guojun ZHENG, Tao MAN, Yangming WANG, Xiaofeng LIU, Jianrong QIU. Optical Properties of Zr4+ Doped CsPbI3 Perovskite Quantum Dots Glass[J]. Journal of the Chinese Ceramic Society, 2024 , 52 (8) : 2606 -2614 . DOI: 10.14062/j.issn.0454-5648.20240108
  • 浙江省自然科学基金(LZ24F050009; LR21E020005)
  • 国家自然科学基金(12304443; 62175210; U20A20211)
  • 区域光纤通信网与新型光通信系统国家重点实验室开放基金(上海交通大学; 2023GZKF016)
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doi: 10.14062/j.issn.0454-5648.20240108
  • 接收时间:2024-02-02
  • 首发时间:2026-10-22
  • 出版时间:2024-08-20
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  • 收稿日期:2024-02-02
  • 修回日期:2024-02-28
基金
浙江省自然科学基金(LZ24F050009; LR21E020005)
国家自然科学基金(12304443; 62175210; U20A20211)
区域光纤通信网与新型光通信系统国家重点实验室开放基金(上海交通大学; 2023GZKF016)
作者信息
    1.浙江工业大学光电子智能化技术研究所,杭州 310023
    2.宁波大学信息科学与工程学院,浙江 宁波 315211
    3.浙江大学光电科学与工程学院,杭州 310027
    4.浙江工业大学计算机科学与技术学院,杭州 310023
    5.浙江大学材料科学与工程学院,杭州 310027

通讯作者:

刘小峰(1982—),男,博士,副教授。
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鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
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红菇属 Russula 17 8.13
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