Article(id=1319971926827713479, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20230644, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1693152000000, receivedDateStr=2023-08-28, revisedDate=1696780800000, revisedDateStr=2023-10-09, acceptedDate=null, acceptedDateStr=null, onlineDate=1792635431248, onlineDateStr=2026-10-22, pubDate=1710864000000, pubDateStr=2024-03-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792635431248, onlineIssueDateStr=2026-10-22, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792635431248, creator=13701087609, updateTime=1792635431248, updator=13701087609, issue=Issue{id=1319971875086783028, tenantId=1146029695717560320, journalId=1263187385517883426, year='2024', volume='52', issue='3', pageStart='737', pageEnd='1170', issueExtLink='null', onlineDate='null', pubDate='1710864000000', pubDateStr='2024-03-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792635418912, creator='13701087609', updateTime=1792641878851, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1319998970110264006, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1319998970110264007, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=845, endPage=852, ext={EN=ArticleExt(id=1319971927477830600, articleId=1319971926827713479, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Effect of Mullite Addition on Microstructure and Optical Property of AlON Transparent Ceramics, columnId=1319726165087077079, journalTitle=Journal of the Chinese Ceramic Society, columnName=Research Article, runingTitle=null, highlight=null, articleAbstract=
Introduction

g-aluminum oxynitride (g-AlON) is widely used for optical lens, transparent arms, and infrared windows due to its high transparency from the ultraviolet to mid-infrared range. To obtain a high-performance AlON transparent ceramic, each stage of its manufacture process should be controlled with cares, i.e., powder synthesis, forming, sintering and annealing. Sintering aid (i.e., Y2O3, CaCO3, Y2O3-La2O3, etc.) is also used to improve the property of AlON transparent ceramic. However, the sintering temperature is still rather high, resulting in a high production cost. Recently, SiO2 is used in AlON system, leading to a decreased temperature of hot isostatic pressing (HIP) (i.e., 1 810 ℃). Unfortunately, however, the evaporation of SiO decomposed from SiO2 could increase the micro-pores in pre-sintered bodies, leading to the density variations and then optical inhomogeneity after HIP. It is thus necessary to explore new Si-contained additive that is stable at a high temperature for the preparation of high-performance AlON transparent ceramics. Mullite (3Al2O3·2SiO2) as a main phase of AlON has a superior high-temperature thermal stability, which is a promising application in AlON system. In this paper, AlON transparent ceramics were fabricated via pressureless sintering and hot isostatic pressing. In addition, the effect of mullite content on the microstructure of pre-sintered and hot isostatic pressed AlON ceramics and their corresponding optical property was also investigated.

Materials and method

An γ-AlON powder with 0.02%-0.20% mullite in alcohol was ground by a planetary mill with high-purity alumina balls. After drying, sieving and then calcining, the mixed powder was pressed into pellets and then cold isostatic pressed to obtain AlON green bodies. The green bodies were pressureless-sintered in a flowing N2 atmosphere at 1 880 ℃ for 4 h, and further hot isostatic pressed in a flowing Ar atmosphere at 1 800 ℃ and 200 MPa for 6 h to obtain AlON transparent ceramics.

The phase analysis of specimens was identified by a model D8 Advance X-ray diffractometer (XRD, Bruker Co., Germany) using nickel-filtered Cu Kα radiation (λ =1.540 6 Å). The bulk density of AlON ceramics was determined by a water immersion method based on Archimedes' principle. The chemically-etched and fracture surfaces of AlON ceramics were characterized by a model TM3000 scanning electron microscope (SEM, Hitachi Co., Japan). The average grain size was determined by a linear intercept line method with a correction factor of 1.56 via a software named Nano Measurer. The Raman spectra were recorded by a model XploRA One-532 Raman spectrometer (Horiba Co., Japan) using a 532 nm Ar+ laser. The optical in-line transmittance spectra of HIPed AlON ceramics were measured by a model V-770 UV-Vis-NIR spectrophotometer (JASCO Co., Japan) and a model FT/IR-4600 Fourier transform infrared spectrometer (FTIR, JASCO Co., Japan).

Results and discussion

The ground AlON powder mixed with mullite has a homogeneous distribution and the particle sizes are in the range of 0.2-1.6 μm with an average value of 0.7 μm. After pressureless sintering, all the XRD patterns of AlON ceramics with 0.02%-0.20% mullite match well with the standard cubic AlON phase (JCPDS 48-0686), and no extra peaks appear, indicating the dissolution of mullite in AlON lattice. The Raman spectraindicate the effect of the mullite content on the structure of the pre-sintered AlON ceramics. The phonon modes located at 316, 372, 628, 764 cm-1 and 920 cm-1 appear in all the samples, which are corresponded to the 3T2g, Eg and A1g modes of spinel. No shift of the Raman bands occurs and new bands do not appear, indicating the same structure and phases in AlON with different mullite contents.

All the pre-sintered AlON ceramics have a milk-white color and are opaque. The microstructure of fracture surfaces indicates that pores easily appear in all the samples. Large pores appear and density decreases in AlON ceramics with 0.10%-0.20% mullite. The grain size increases steadily with increasing mullite content. For the low content and high-temperature stability of mullite, a reaction of solid-state sintering is proposed as . Furthermore, for an oxygen-rich AlON phase in the formation of AlON, the covalent bond strength of Al-N is higher than that of Al-O, and the diffusivity of oxygen is faster than that of nitrogen. AlON with a higher Al2O3 content is easy to sintering, leading to the grain growth. Al2O3 content increases and grains grow with increasing mullite content. The grains grow fast at a high mullite content, resulting in some trapped pores within the grains.

All the hot isostatic pressed AlON ceramics have a density of > 99.2% of the theoretical value and a high transparency. The density, grain size and transmittance of hot isostatic pressed AlON ceramic firstly increase and then decrease with increasing mullite content. AlON transparent ceramic doped with 0.05% mullite exhibits the maximum transmittance of 81.9% (4 mm thickness) at 2 000 nm, with a density of 3.67 g/cm3 and an average grain size of 80.4 μm. Some pores in the grains appear in pre-sintered bodies at a higher mullite content, inhibiting the grain growth during the HIP process and desceasing the grain size. Also, some pores in the grains cannot eliminate and remain after HIP, degrading the transmittance.

Conclusions

AlON transparent ceramics were fabricated via pressureless sintering at 1 880 ℃ and hot isostatic pressing (HIP) at 1 800 ℃, respectively, with AlON powder and mullite., The same structure of AlON with different mullite contents of 0.02%-0.20% could be obtained. AlON transparent ceramic with 0.05% mullite exhibited the maximum transmittance of 81.9% (4 mm thickness) at 2 000 nm. At a mullite content of > 0.10%, some pores in grains appeared in pre-sintered bodies, inhibiting the grain growth in the HIP process.

, authors=Rongwei SHI1, 2, Liqiong AN1, Xiaojian MAO2, Buhao ZHANG2, 3, Jianmin LI2, Jian ZHANG2, Shiwei WANG2, authorsList=Rongwei SHI, Liqiong AN, Xiaojian MAO, Buhao ZHANG, Jianmin LI, Jian ZHANG, Shiwei WANG, authorCompany=null, correspAuthors=Liqiong AN, Xiaojian MAO, authorNote=

SHI Rongwei (1997-), male, Master candidate. E-mail:

, correspAuthorsNote=
AN Liqiong (1979-), female, Ph.D., Associate Professor; E-mail: ;
MAO Xiaojian (1980-), male, Ph.D., Professor.
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以自制AlON粉体为原料、莫来石为烧结助剂,结合无压烧结与热等静压烧结在相对较低的温度下(分别为1 880 ℃和1 800 ℃)制备了AlON透明陶瓷,研究了莫来石含量对无压烧结和热等静压烧结AlON陶瓷的显微结构以及光学性能的影响。结果表明,莫来石含量在0.02%~0.20%(质量分数)时,无压烧结AlON陶瓷为纯AlON相,其Raman光谱相似。随着莫来石含量增加,AlON陶瓷无压预烧体的致密度先增加后减小,而其晶粒尺寸逐渐变大。热等静压烧结后,所有样品的致密度均高于理论密度的99.2%且晶粒长大;其致密度、晶粒和透过率随莫来石含量增加呈现出先增大后减小的趋势。最终,0.05%莫来石AlON透明陶瓷致密度为3.67 g/cm3,平均晶粒尺寸为80.4 μm,其透过率最高,4 mm厚样品在2 000 nm处达到81.9%。

, authors=史镕玮1, 2, 安丽琼1, 毛小建2, 张步豪2, 3, 李建民2, 章健2, 王士维2, authorsList=史镕玮, 安丽琼, 毛小建, 张步豪, 李建民, 章健, 王士维, authorCompany=null, correspAuthors=安丽琼, 毛小建, authorNote=

史镕玮(1997—),男,硕士研究生。

, correspAuthorsNote=
安丽琼(1979—),女,博士,副教授;
毛小建(1980—),男,博士,研究员。
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莫来石助剂对氧氮化铝透明陶瓷显微结构及光学性能的影响
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史镕玮 1, 2 , 安丽琼 1 , 毛小建 2 , 张步豪 2, 3 , 李建民 2 , 章健 2 , 王士维 2
硅酸盐学报 | 研究论文 2024,52(3): 845-852
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硅酸盐学报 |研究论文 2024 , 52 (3) : 845 -852
莫来石助剂对氧氮化铝透明陶瓷显微结构及光学性能的影响
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史镕玮1, 2 , 安丽琼1 , 毛小建2 , 张步豪2, 3, 李建民2, 章健2, 王士维2
作者信息
  • 1.上海海事大学海洋科学与工程学院,上海,201306,中国
  • 2.中国科学院上海硅酸盐研究所国家重点实验室,上海 200050,中国
  • 3.英国诺丁汉大学工程学院,诺丁汉,NG7 2RD,英国
通讯作者:
安丽琼(1979—),女,博士,副教授;
毛小建(1980—),男,博士,研究员。
作者简介:

史镕玮(1997—),男,硕士研究生。

Effect of Mullite Addition on Microstructure and Optical Property of AlON Transparent Ceramics
Rongwei SHI1, 2 , Liqiong AN1 , Xiaojian MAO2 , Buhao ZHANG2, 3, Jianmin LI2, Jian ZHANG2, Shiwei WANG2
Affiliations
  • 1.College of Ocean Science and Engineering, Shanghai Maritime University, Shanghai, 201306, China
  • 2.State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, 200050, China
  • 3.Faculty of Engineering, University of Nottingham, Nottingham, NG7 2RD, United Kingdom
  • Corresponding Author:
    AN Liqiong (1979-), female, Ph.D., Associate Professor; E-mail: ;
    MAO Xiaojian (1980-), male, Ph.D., Professor.

    SHI Rongwei (1997-), male, Master candidate. E-mail:

出版时间: 2024-03-20 doi: 10.14062/j.issn.0454-5648.20230644
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以自制AlON粉体为原料、莫来石为烧结助剂,结合无压烧结与热等静压烧结在相对较低的温度下(分别为1 880 ℃和1 800 ℃)制备了AlON透明陶瓷,研究了莫来石含量对无压烧结和热等静压烧结AlON陶瓷的显微结构以及光学性能的影响。结果表明,莫来石含量在0.02%~0.20%(质量分数)时,无压烧结AlON陶瓷为纯AlON相,其Raman光谱相似。随着莫来石含量增加,AlON陶瓷无压预烧体的致密度先增加后减小,而其晶粒尺寸逐渐变大。热等静压烧结后,所有样品的致密度均高于理论密度的99.2%且晶粒长大;其致密度、晶粒和透过率随莫来石含量增加呈现出先增大后减小的趋势。最终,0.05%莫来石AlON透明陶瓷致密度为3.67 g/cm3,平均晶粒尺寸为80.4 μm,其透过率最高,4 mm厚样品在2 000 nm处达到81.9%。

氧氮化铝  /  透明陶瓷  /  烧结助剂  /  莫来石  /  热等静压
Introduction

g-aluminum oxynitride (g-AlON) is widely used for optical lens, transparent arms, and infrared windows due to its high transparency from the ultraviolet to mid-infrared range. To obtain a high-performance AlON transparent ceramic, each stage of its manufacture process should be controlled with cares, i.e., powder synthesis, forming, sintering and annealing. Sintering aid (i.e., Y2O3, CaCO3, Y2O3-La2O3, etc.) is also used to improve the property of AlON transparent ceramic. However, the sintering temperature is still rather high, resulting in a high production cost. Recently, SiO2 is used in AlON system, leading to a decreased temperature of hot isostatic pressing (HIP) (i.e., 1 810 ℃). Unfortunately, however, the evaporation of SiO decomposed from SiO2 could increase the micro-pores in pre-sintered bodies, leading to the density variations and then optical inhomogeneity after HIP. It is thus necessary to explore new Si-contained additive that is stable at a high temperature for the preparation of high-performance AlON transparent ceramics. Mullite (3Al2O3·2SiO2) as a main phase of AlON has a superior high-temperature thermal stability, which is a promising application in AlON system. In this paper, AlON transparent ceramics were fabricated via pressureless sintering and hot isostatic pressing. In addition, the effect of mullite content on the microstructure of pre-sintered and hot isostatic pressed AlON ceramics and their corresponding optical property was also investigated.

Materials and method

An γ-AlON powder with 0.02%-0.20% mullite in alcohol was ground by a planetary mill with high-purity alumina balls. After drying, sieving and then calcining, the mixed powder was pressed into pellets and then cold isostatic pressed to obtain AlON green bodies. The green bodies were pressureless-sintered in a flowing N2 atmosphere at 1 880 ℃ for 4 h, and further hot isostatic pressed in a flowing Ar atmosphere at 1 800 ℃ and 200 MPa for 6 h to obtain AlON transparent ceramics.

The phase analysis of specimens was identified by a model D8 Advance X-ray diffractometer (XRD, Bruker Co., Germany) using nickel-filtered Cu Kα radiation (λ =1.540 6 Å). The bulk density of AlON ceramics was determined by a water immersion method based on Archimedes' principle. The chemically-etched and fracture surfaces of AlON ceramics were characterized by a model TM3000 scanning electron microscope (SEM, Hitachi Co., Japan). The average grain size was determined by a linear intercept line method with a correction factor of 1.56 via a software named Nano Measurer. The Raman spectra were recorded by a model XploRA One-532 Raman spectrometer (Horiba Co., Japan) using a 532 nm Ar+ laser. The optical in-line transmittance spectra of HIPed AlON ceramics were measured by a model V-770 UV-Vis-NIR spectrophotometer (JASCO Co., Japan) and a model FT/IR-4600 Fourier transform infrared spectrometer (FTIR, JASCO Co., Japan).

Results and discussion

The ground AlON powder mixed with mullite has a homogeneous distribution and the particle sizes are in the range of 0.2-1.6 μm with an average value of 0.7 μm. After pressureless sintering, all the XRD patterns of AlON ceramics with 0.02%-0.20% mullite match well with the standard cubic AlON phase (JCPDS 48-0686), and no extra peaks appear, indicating the dissolution of mullite in AlON lattice. The Raman spectraindicate the effect of the mullite content on the structure of the pre-sintered AlON ceramics. The phonon modes located at 316, 372, 628, 764 cm-1 and 920 cm-1 appear in all the samples, which are corresponded to the 3T2g, Eg and A1g modes of spinel. No shift of the Raman bands occurs and new bands do not appear, indicating the same structure and phases in AlON with different mullite contents.

All the pre-sintered AlON ceramics have a milk-white color and are opaque. The microstructure of fracture surfaces indicates that pores easily appear in all the samples. Large pores appear and density decreases in AlON ceramics with 0.10%-0.20% mullite. The grain size increases steadily with increasing mullite content. For the low content and high-temperature stability of mullite, a reaction of solid-state sintering is proposed as . Furthermore, for an oxygen-rich AlON phase in the formation of AlON, the covalent bond strength of Al-N is higher than that of Al-O, and the diffusivity of oxygen is faster than that of nitrogen. AlON with a higher Al2O3 content is easy to sintering, leading to the grain growth. Al2O3 content increases and grains grow with increasing mullite content. The grains grow fast at a high mullite content, resulting in some trapped pores within the grains.

All the hot isostatic pressed AlON ceramics have a density of > 99.2% of the theoretical value and a high transparency. The density, grain size and transmittance of hot isostatic pressed AlON ceramic firstly increase and then decrease with increasing mullite content. AlON transparent ceramic doped with 0.05% mullite exhibits the maximum transmittance of 81.9% (4 mm thickness) at 2 000 nm, with a density of 3.67 g/cm3 and an average grain size of 80.4 μm. Some pores in the grains appear in pre-sintered bodies at a higher mullite content, inhibiting the grain growth during the HIP process and desceasing the grain size. Also, some pores in the grains cannot eliminate and remain after HIP, degrading the transmittance.

Conclusions

AlON transparent ceramics were fabricated via pressureless sintering at 1 880 ℃ and hot isostatic pressing (HIP) at 1 800 ℃, respectively, with AlON powder and mullite., The same structure of AlON with different mullite contents of 0.02%-0.20% could be obtained. AlON transparent ceramic with 0.05% mullite exhibited the maximum transmittance of 81.9% (4 mm thickness) at 2 000 nm. At a mullite content of > 0.10%, some pores in grains appeared in pre-sintered bodies, inhibiting the grain growth in the HIP process.

aluminum oxynitride  /  transparent ceramic  /  sintering aid  /  mullite  /  hot isostatic pressing
史镕玮, 安丽琼, 毛小建, 张步豪, 李建民, 章健, 王士维. 莫来石助剂对氧氮化铝透明陶瓷显微结构及光学性能的影响. 硅酸盐学报, 2024 , 52 (3) : 845 -852 . DOI: 10.14062/j.issn.0454-5648.20230644
Rongwei SHI, Liqiong AN, Xiaojian MAO, Buhao ZHANG, Jianmin LI, Jian ZHANG, Shiwei WANG. Effect of Mullite Addition on Microstructure and Optical Property of AlON Transparent Ceramics[J]. Journal of the Chinese Ceramic Society, 2024 , 52 (3) : 845 -852 . DOI: 10.14062/j.issn.0454-5648.20230644
  • 国家自然科学基金(51902330)
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doi: 10.14062/j.issn.0454-5648.20230644
  • 接收时间:2023-08-28
  • 首发时间:2026-10-22
  • 出版时间:2024-03-20
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  • 收稿日期:2023-08-28
  • 修回日期:2023-10-09
基金
国家自然科学基金(51902330)
作者信息
    1.上海海事大学海洋科学与工程学院,上海,201306,中国
    2.中国科学院上海硅酸盐研究所国家重点实验室,上海 200050,中国
    3.英国诺丁汉大学工程学院,诺丁汉,NG7 2RD,英国

通讯作者:

安丽琼(1979—),女,博士,副教授;
毛小建(1980—),男,博士,研究员。
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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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