Article(id=1320107625610589151, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320107605469544753, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20250683, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1757952000000, receivedDateStr=2025-09-16, revisedDate=1762099200000, revisedDateStr=2025-11-03, acceptedDate=null, acceptedDateStr=null, onlineDate=1792667784358, onlineDateStr=2026-10-22, pubDate=1787155200000, pubDateStr=2026-08-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792667784358, onlineIssueDateStr=2026-10-22, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792667784358, creator=13701087609, updateTime=1792667784358, updator=13701087609, issue=Issue{id=1320107605469544753, tenantId=1146029695717560320, journalId=1263187385517883426, year='2026', volume='54', issue='9', pageStart='2949', pageEnd='3314', issueExtLink='null', onlineDate='null', pubDate='1789833600000', pubDateStr='2026-09-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792667779556, creator='13701087609', updateTime=1792737576818, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1320400356446687492, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320107605469544753, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1320400356446687493, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1320107605469544753, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=3161, endPage=3172, ext={EN=ArticleExt(id=1320107625811915744, articleId=1320107625610589151, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Influences of Yb
3+ Content on Microstructures and Properties of Yb∶Lu
2O
3 Transparent Ceramics, columnId=1263922769897599102, journalTitle=Journal of the Chinese Ceramic Society, columnName=Research Articles, runingTitle=null, highlight=null, articleAbstract=
Introduction Lutetium oxide (Lu2O3) transparent ceramics have a great potential in high-power or high-efficiency solid-state laser applications due to the excellent thermal-mechanical properties, low fabrication temperature, high absorption and emission cross-sections when doped with trivalent rare earth laser ions. Among them, Lu2O3 doped with Yb3+ stands out as the best combination for applications in high-efficiency and high-power lasers, considering a high thermal conductivity due to the similar ionic radii and bonding forces of lutetium and ytterbium ions. The combination of vacuum pre-sintering with HIP post-treatment, along with the powder synthesized by a co-precipitation method, highly favors to fabricate highly transparent sesquioxide ceramics. Some previous reports demonstrated the high efficiency and high power laser outputs of Yb:Lu2O3 transparent ceramics. Thermal properties of Yb:Lu2O3 ceramics are significant for the high-efficiency and high-power laser applications. In ceramic gain media, the significant factors affecting the thermal conductivity include the doping content of active ions, porosity and grain size. Although increasing Yb3+ concentration could not cause a decrease in thermal conductivity in theory, little work has reported the related experimental investigations yet.
Methods The commercial oxide powders (i.e., Lu2O3 and Yb2O3) were utilized as raw materials. Ammonium bicarbonate (NH4HCO3) and ammonium sulfate ((NH4)2SO4) were used as a precipitant and a dispersant, respectively. The precursors of Yb:Lu2O3 were synthesized by a co-precipitation method. All the precursors with different Yb3+ doping contents were calcined at 1050 ℃ to obtain Yb:Lu2O3 powders, which were dry-pressed at a low pressure in a steel die and then cold-isostatically pressed at 250 MPa. All the green bodies were vacuum sintered at 1500 ℃ for 2 h to fabricate pre-sintered ceramics that then were HIP post-treated in Ar atmosphere pressure of 176 MPa at 1750 ℃ for 3 h. Finally, the HIP post-treated ceramics were annealed in air at 900 ℃ for 10 h and then polished on the both sides to a thickness of 1.3 mm for the coming optical characterizations. Some annealed transparent ceramic disks were then machined to the sizes of (Φ = 10.0 mm, d = 1.3 mm) and (Φ=5.5 mm, d<1.0 mm) for measuring the thermal diffusivity and specific heat, respectively.
The phase compositions of the synthesized precursors and powders were identified by X-ray diffraction (XRD, Cu Kα1 radiation, λ = 0.154 18 nm). The microstructures of all the powders and ceramics were determined by field emission scanning electron microscopy (FESEM, SU8220, Hitachi, Japan). The in-line transmittance and absorption spectra of Yb∶Lu2O3 transparent ceramics were characterized by ultraviolet-visible-near infrared spectroscopy (UV-VIS-NIR, Carry-5000, Varian, USA). The thermal diffusivity was measured by a laser-flash method, and the specific heat was measured by differential scanning calorimetry (DSC).
Results and discussion Pure Lu2O3 precursor consists of spherical particles with various sizes, which range from tens of nanometers to hundreds of nanometers in diameter, but the micro-morphology of the precursor with Yb3+ is made of thin stacked layers with nano-sized thickness, indicating that Yb3+ doping has a great impact on the morphologies of Lu2O3 precursor, but its concentration level does not affect the morphologies of the precursors apparently. The particles of Yb3+-doped nano-powders agglomerate in two-dimensional space and are in the shape of regular polyhedra. The phases of all the calcined nano-powders are consistent with those of cubic Lu2O3. The lattice parameters of Yb:Lu2O3 nano-powders are 10.384 4、10.389 4、10.390 2、10.394 9 Åand 10.396 5 Å, respectively, with increasing the Yb3+ concentration. The corresponding average gain sizes are 57.7, 51.9, 53.6, 61.8 and 51.4 nm, respectively. The relative densities of all the Yb:Lu2O3 pre-sintered ceramics are 95.3%, 96.1%, 95.6%, 95.4% and 95.7%, with average grain sizes of 0.92, 0.97, 0.99, 1.09 μm and 1.14 μm, respectively, as Yb3+ concentration increases. 3% Yb:Lu2O3 transparent ceramic sample has the maximum in-line transmittance with the values of 83.0% at 1080 nm and 78.8% at 600 nm. The absorption coefficients at 948 nm of these ceramics are linearly correlated to Yb3+ doping content, which follows the Lambert-Beer Law. Four main emission peaks are located at 948, 976, 1033 and 1079 nm, respectively, among which the largest emission cross-section is at 976 nm with a value of 1.148×10-20 cm2. The laser emission wavelengths include 1079 nm and 1033 nm. The maximum thermal conductivity of 3% Yb∶Lu2O3 ceramics is 13.1 W·m-1·K-1 at room temperature, which is similar to the value of Yb:Lu2O3 single crystal, while the thermal conductivity of 15% Yb∶Lu2O3 ceramics is 11.6 W·m-1·K-1, which is greater than that of pure YAG material. The result indicates that Yb:Lu2O3 transparent ceramics are a gain medium with a high thermal conductivity, even doped with a high Yb3+ doping content, demonstrating a great application potential in high-power solid-state lasers.
Conclusions Yb:Lu2O3 transparent ceramics with Yb3+ doping content of 0-15% were fabricated by vacuum sintering and HIP post-treating from co-precipitated nano-powders. The nano-powders calcined at 1050 ℃ had the similar particle sizes with different morphologies as the precursors. 3% Yb∶Lu2O3 nano-powder showed a better dispersivity, and the corresponding transparent ceramics possessed the maximum optical quality with the in-line transmittance of 83% at 1080 nm. The spectral characteristics of all the Yb:Lu2O3 transparent ceramics were calculated. At β of > 0.059, there were two main lasing emission wavelengths, peaked at 1033 nm and 1079 nm, respectively. 3% Yb:Lu2O3 transparent ceramics possessed better thermal properties rather than others, with the room-temperature thermal conductivity of 13.1 W·m-1·K-1. The results indicated a great application potential of Yb:Lu2O3 transparent ceramics in high-power solid-state lasers.
, authors=Ziyu LIU
1, 2, Yagang FENG
3, Peng LIU
1, Chen HU
2, 4, Congcong LIU
1, Wenwen ZHENG
1, Xianfeng YANG
1, Jiang LI
2, 4, authorsList=Ziyu LIU, Yagang FENG, Peng LIU, Chen HU, Congcong LIU, Wenwen ZHENG, Xianfeng YANG, Jiang LI, authorCompany=null, correspAuthors=Xianfeng YANG, Jiang LI, authorNote=
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3+含量对Yb:Lu
2O
3透明陶瓷微观结构与性能的影响, columnId=1263922770220560512, journalTitle=硅酸盐学报, columnName=研究论文, runingTitle=null, highlight=null, articleAbstract=
镱掺杂氧化镥(Yb:Lu2O3)透明陶瓷由于具有热导率高、抗热震性能优异、高吸收与发射截面和远低于熔点的制备温度等优势备受关注。本工作以共沉淀法合成的纳米粉体为原料,采用真空预烧结合热等静压(HIP)后处理工艺制备了不同Yb3+掺杂量的Yb∶Lu2O3透明陶瓷,系统研究了镱离子(Yb3+)掺杂量对粉体形貌与物相及陶瓷微观结构、光学质量、光谱特性和热学性能的影响。其中,3%(Yb3+的摩尔分数)Yb∶Lu2O3陶瓷直线透过率最佳,在1080 nm处为83.0%。不同陶瓷中Yb3+的吸收系数与掺杂量呈线性相关,可推断Yb3+基本进入了Lu2O3晶格;且Yb∶Lu2O3透明陶瓷的吸收和发射截面与单晶相当。室温下,3%和15% Yb∶Lu2O3透明陶瓷的热导率分别约为13.1 W·m-1·K-1和11.6 W·m-1·K-1,说明高浓度Yb3+掺杂的Yb∶Lu2O3透明陶瓷具有优良热学性能,是非常有前景的1 μm高功率固态激光增益介质。
, authors=刘子玉
1, 2, 冯亚刚
3, 刘鹏
1, 胡辰
2, 4, 刘聪聪
1, 郑雯雯
1, 杨现锋
1, 李江
2, 4, authorsList=刘子玉, 冯亚刚, 刘鹏, 胡辰, 刘聪聪, 郑雯雯, 杨现锋, 李江, authorCompany=null, correspAuthors=杨现锋, 李江, authorNote=
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杨现锋(1980—),男,博士,教授;
李江(1977—),男,博士,研究员。
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1.School of Materials Science and Engineering, Changsha University of Science & Technology, Changsha 410114, China
2.Transparent Ceramics Research Center, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201899, China, bio={"content":"
LIU Ziyu (1991-), female, Ph.D., Lecturer. E-mail: ziyuliu@csust.edu.cn
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1.长沙理工大学材料科学与工程学院,长沙 410114
2.中国科学院上海硅酸盐研究所透明陶瓷研究中心,上海 201899, bio={"content":"
刘子玉(1991—),女,博士,讲师。
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3.School of Materials Science and Engineering, Henan University of Technology, Zhengzhou 450007, China, bio=null, bioImg=null, bioContent=null, aboutCorrespAuthor=null), CN=AuthorExt(id=1320107627141510136, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, authorId=1320107626965349365, language=CN, stringName=冯亚刚, firstName=null, middleName=null, lastName=null, prefix=null, suffix=null, authorComment=null, nameInitials=null, affiliation=null, department=null, xref=
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3.河南工业大学材料科学与工程学院,郑州 450001, bio=null, bioImg=null, bioContent=null, aboutCorrespAuthor=null)}, companyList=[AuthorCompany(id=1320107626487198696, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, xref=3., ext=[AuthorCompanyExt(id=1320107626495587305, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, companyId=1320107626487198696, language=EN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=
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3.河南工业大学材料科学与工程学院,郑州 450001)])]), Author(id=1320107627212813306, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, orderNo=2, firstName=null, middleName=null, lastName=null, nameCn=null, orcid=null, stid=null, country=null, authorPic=null, dead=0, email=null, emailSecond=null, emailThird=null, correspondingAuthor=0, authorType=1, ext={EN=AuthorExt(id=1320107627275727868, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, authorId=1320107627212813306, language=EN, stringName=Peng LIU, firstName=Peng, middleName=null, lastName=LIU, prefix=null, suffix=null, authorComment=null, nameInitials=null, affiliation=null, department=null, xref=
1, address=
1.School of Materials Science and Engineering, Changsha University of Science & Technology, Changsha 410114, China, bio=null, bioImg=null, bioContent=null, aboutCorrespAuthor=null), CN=AuthorExt(id=1320107627338642429, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, authorId=1320107627212813306, language=CN, stringName=刘鹏, firstName=null, middleName=null, lastName=null, prefix=null, suffix=null, authorComment=null, nameInitials=null, affiliation=null, department=null, xref=
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1.长沙理工大学材料科学与工程学院,长沙 410114, bio=null, bioImg=null, bioContent=null, aboutCorrespAuthor=null)}, companyList=[AuthorCompany(id=1320107626311037922, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, xref=1., ext=[AuthorCompanyExt(id=1320107626319426531, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, companyId=1320107626311037922, language=EN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=
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2, 4, address=
2.Transparent Ceramics Research Center, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201899, China
4.Center of Materials Science and Optoelectronic Technology, University of Chinese Academy of Sciences, Beijing 100049, China, bio=null, bioImg=null, bioContent=null, aboutCorrespAuthor=null), CN=AuthorExt(id=1320107627607076866, tenantId=1146029695717560320, journalId=1263187385517883426, articleId=1320107625610589151, authorId=1320107627447694335, language=CN, stringName=胡辰, firstName=null, middleName=null, lastName=null, prefix=null, suffix=null, authorComment=null, nameInitials=null, affiliation=null, department=null, xref=
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2.中国科学院上海硅酸盐研究所透明陶瓷研究中心,上海 201899
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