{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"用湿化学方法合成了Ce<span style=\"color:red\">3</span>+/Dy<span style=\"color:red\">3</span>+及Ce<span style=\"color:red\">3</span>+/Tb<span style=\"color:red\">3</span>+共掺<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>发光材料.利用X射线衍射仪对其进行了物相分析,结果表明:合成物为纯的六方相<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>微晶.利用荧光分光光谱仪进行光谱分析,测定了合成样品的激发和发射光谱.发现在紫外激发下,<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Dy荧光粉发射出很强的偏黄的白光,其发射峰分别位于480,575和665 nm,对应于Dy<span style=\"color:red\">3</span>+的<span style=\"color:red\">4</span>F9/2→6H15/2,13/2,11/2跃迁.掺Ce<span style=\"color:red\">3</span>+对Dy<span style=\"color:red\">3</span>+起到敏化作用,<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Dy,Ce发出很亮的暖白光,且强度是<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Dy的<span style=\"color:red\">3</span>倍左右.同时,在Ce<span style=\"color:red\">3</span>+/Tb<span style=\"color:red\">3</span>+共掺的样品中,由于Ce<span style=\"color:red\">3</span>+与Tb<span style=\"color:red\">3</span>+间的能量传递,Tb<span style=\"color:red\">3</span>+的541 nm特征峰显著增强.","authors":[{"authorName":"杨成浩","id":"caa5179d-cf97-4676-8500-bb8c0df00091","originalAuthorName":"杨成浩"},{"authorName":"潘跃晓","id":"2da918fd-6d06-4557-9335-009e202a211a","originalAuthorName":"潘跃晓"},{"authorName":"张勤远","id":"443ca35c-84ff-4aa5-9dd9-cc4736f4b8a1","originalAuthorName":"张勤远"}],"doi":"","fpage":"568","id":"a5d8dda4-d1fb-4987-be29-2fb1e046def1","issue":"z2","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"9ea2b9d5-d1e4-42eb-af59-17745ff1071d","keyword":"湿化学法","originalKeyword":"湿化学法"},{"id":"aed6097d-9082-4008-8516-5bdaffc7f4b4","keyword":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>","originalKeyword":"GdAl3(BO3)4"},{"id":"0f6eb20f-aa0e-4662-a414-cd9ac929f119","keyword":"荧光粉","originalKeyword":"荧光粉"},{"id":"608791ae-3f9b-491a-9ad4-5f7f13130865","keyword":"光致发光","originalKeyword":"光致发光"}],"language":"zh","publisherId":"xyjsclygc2008z2149","title":"Ce<span style=\"color:red\">3</span>+掺杂对<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Dy<span style=\"color:red\">3</span>+和<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Tb<span style=\"color:red\">3</span>+荧光粉发光性能的影响","volume":"37","year":"2008"},{"abstractinfo":"用硝酸盐热分解法合成了单相粉末样品Gd1-xEuxAl<span style=\"color:red\">3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>(0≤x≤1).研究了Eu<span style=\"color:red\">3</span>+在<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>中的紫外和真空紫外光谱性质.<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Eu<span style=\"color:red\">3</span>+中稀土离子占据非中心对称的格位,Eu<span style=\"color:red\">3</span>+在其中的特征发射以5Do→7F2电偶极跃迁为主.在147nm激发下<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Eu<span style=\"color:red\">3</span>+呈色坐标为(0.645,0.330)的强红光发射,说明是非常有前途的PDP用红色发光材料.在<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Eu<span style=\"color:red\">3</span>+的真空紫外光谱中观察到两个峰,158nm的激发带归属于<span style=\"color:red\">BO3</span>基团的吸收,258nm处的激发带为Eu<span style=\"color:red\">3</span>+→O2-的电荷转移跃迁带.在147nm激发下,<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Eu<span style=\"color:red\">3</span>+的红光发射强度随着Eu<span style=\"color:red\">3</span>+浓度的增加而减弱,而在258nm激发下随Eu<span style=\"color:red\">3</span>+浓度的增大Eu<span style=\"color:red\">3</span>+的红光发射增强,说明它们发光的机理不同.","authors":[{"authorName":"王育华","id":"b38530fc-d39d-475c-94bc-a19793ccaf25","originalAuthorName":"王育华"},{"authorName":"远滕忠","id":"9422ebb7-aad3-440f-92db-899e38d21589","originalAuthorName":"远滕忠"},{"authorName":"都云昆","id":"ebda8489-574a-4a31-827e-031d08405f74","originalAuthorName":"都云昆"}],"doi":"10.3321/j.issn:1000-324X.2004.04.011","fpage":"772","id":"3c5193e9-3c10-4cc9-99de-006e8303c916","issue":"4","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"671681f6-d0ee-45d0-9dc1-cd30d53ae00a","keyword":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>","originalKeyword":"GdAl3(BO3)4"},{"id":"fafeed25-4d74-4d18-aa5b-8ad4c3968d29","keyword":"发光","originalKeyword":"发光"},{"id":"0512350a-0605-4c9a-b765-0092a86e6988","keyword":"紫外及真空紫外光谱","originalKeyword":"紫外及真空紫外光谱"}],"language":"zh","publisherId":"wjclxb200404011","title":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>:Eu<span style=\"color:red\">3</span>+荧光粉的光致发光特性","volume":"19","year":"2004"},{"abstractinfo":"用硝酸盐热分解法合成了单相粉末样品Gd<SUB>1-<EM>x</EM></SUB>Eu<SUB><EM>x</EM></SUB>Al<SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>(0≤<EM>x</EM>≤1)。研究了Eu<SUP><span style=\"color:red\">3</span>+</SUP>在<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>中的紫外和真空紫外光谱性质。<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>:Eu<SUP><span style=\"color:red\">3</span>+</SUP>中稀土离子占据非中心对称的格位,Eu<SUP><span style=\"color:red\">3</span>+</SUP>在其中的特征发射以<SUP>5</SUP><EM>D</EM><SUB>0</SUB>→<SUP>7</SUP><EM>F</EM><SUB>2</SUB>电偶极跃迁为主。在147nm激发下<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>:Eu<SUP><span style=\"color:red\">3</span>+</SUP>呈色坐标为(0.645,0.330)的强红光发射,说明是非常有前途的PDP用红色发光材料。在GdA<SUB>l<span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>:Eu<SUP><span style=\"color:red\">3</span>+</SUP>的真空紫外光谱中观察到两个峰,158nm的激发带归属于<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>基团的吸收,258nm处的激发带为Eu<SUP><span style=\"color:red\">3</span>+</SUP>→O<SUP>2-</SUP>的电荷转移跃迁带。在147nm激发下,<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>:Eu<SUP><span style=\"color:red\">3</span>+</SUP>的红光发射强度随着Eu<SUP><span style=\"color:red\">3</span>+</SUP>浓度的增加而减弱,而在258nm激发下随Eu<SUP><span style=\"color:red\">3</span>+</SUP>浓度的增大Eu<SUP><span style=\"color:red\">3</span>+</SUP>的红光发射增强,说明它们发光的机理不同。","authors":[{"authorName":"王育华","id":"d602fce2-1768-47bd-90f3-807977e6326f","originalAuthorName":"王育华"},{"authorName":"远滕忠","id":"a2e125be-89ac-4df8-b1ea-ac899c909cb2","originalAuthorName":"远滕忠"},{"authorName":"都云昆","id":"239c73ec-2b73-4ecf-bfa5-2e6176ce3a1b","originalAuthorName":"都云昆"}],"categoryName":"|","doi":"","fpage":"772","id":"5743c97d-82c5-471d-996b-0c6f601ce4dc","issue":"4","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"9e13a097-d682-4fb8-8cc1-72f208da63a1","keyword":"<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>（<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>）<SUB><span style=\"color:red\">4</span></SUB>","originalKeyword":"GdAl<SUB>3</SUB>（BO<SUB>3</SUB>）<SUB>4</SUB>"},{"id":"2a81f378-4ece-432d-b172-e40cf57d67bb","keyword":" luminescence","originalKeyword":" luminescence"},{"id":"e254a7a3-3ccd-4c45-88a7-5d29c4f094b3","keyword":" UV","originalKeyword":" UV"}],"language":"zh","publisherId":"1000-324X_2004_4_36","title":"<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>:Eu<SUP><span style=\"color:red\">3</span>+</SUP>荧光粉的光致发光特性","volume":"19","year":"2004"},{"abstractinfo":"采用顶部籽晶法从K2Mo<span style=\"color:red\">3O10-B2O3</span>助熔剂体系中生长出尺寸达到20 mm的<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>(简称GAB)和Yb<span style=\"color:red\">3</span>+激活的晶体.测试了GAB晶体的<100>和(001)轴向热膨胀系数,确定了透光波长范围,计算了有效倍频系数和相位匹配角随波长的变化,结果表明GAB晶体在整个透光范围内均可实现相位匹配.测定了Yb<span style=\"color:red\">3</span>+:GAB晶体在室温下的偏振吸收和荧光光谱,进行了光谱计算,测试了晶体的激光性能,在1046 nm处实现了2.1 W激光输出,斜率效率达到58%.","authors":[{"authorName":"朱昭捷","id":"8cc35dad-2c8f-4219-81ec-4457894b868d","originalAuthorName":"朱昭捷"},{"authorName":"李坚富","id":"58f041c1-eac1-4b99-a215-c1bea84e3d20","originalAuthorName":"李坚富"},{"authorName":"吴柏昌","id":"903f0871-bd2d-4210-8ed5-ac3f62746f7b","originalAuthorName":"吴柏昌"},{"authorName":"游振宇","id":"ac6dc726-218f-4726-8d1b-5eef4482d903","originalAuthorName":"游振宇"},{"authorName":"王燕","id":"06f9b534-ab56-45cf-beba-4edc485a559b","originalAuthorName":"王燕"},{"authorName":"马兴华","id":"0daea53c-c094-478b-ade4-8f4b03b49774","originalAuthorName":"马兴华"},{"authorName":"涂朝阳","id":"e6c69df6-c2d2-4076-9c41-a781568bcc94","originalAuthorName":"涂朝阳"},{"authorName":"","id":"a322a7fc-c4f0-4ad7-89a1-8366e2e75b64","originalAuthorName":""}],"doi":"","fpage":"507","id":"2fa9fcc5-4dd9-4a39-b2c1-6a5ace6d28a3","issue":"3","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"252db340-7488-426e-b6e9-dc896694b73f","keyword":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>晶体","originalKeyword":"GdAl3(BO3)4晶体"},{"id":"03aace94-6f29-4b4b-9575-6fa211d3d18f","keyword":"Yb<span style=\"color:red\">3</span>+离子","originalKeyword":"Yb3+离子"},{"id":"0ffcacba-7110-442c-9418-0a1ecaadb9a2","keyword":"光谱性能","originalKeyword":"光谱性能"},{"id":"9890bf3c-8b11-44bc-b1ea-2b6622c7f97b","keyword":"激光性能","originalKeyword":"激光性能"}],"language":"zh","publisherId":"rgjtxb98200803001","title":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>及其Yb<span style=\"color:red\">3</span>+激活激光晶体的研究","volume":"37","year":"2008"},{"abstractinfo":"采用熔盐法生长出尺寸为30mm的Nd<SUP><span style=\"color:red\">3</span>+</SUP>:<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>优质晶体,进行了吸收光谱和荧光光谱的测定研究,计算得到晶体发射截面为σ<SUB>e</SUB><SUP>1061.9</SUP>=2.9×10<SUP>-19</SUP>cm<SUP>2</SUP>和σ<SUB>e</SUB><SUP>1338mm</SUP>=5.5×10<SUP>-20</SUP>cm<SUP>2</SUP>.采用染料激光器作为泵浦源,对晶体进行了自变频激光实验研究,在紫外可调谐(378-382nm)、绿光531nm、蓝光(436-443nm)、红光(669nm)和红外可调谐(1305-1365nm)波段实现了激光输出,输出的最大功率分别为:105μJ/脉冲、119.5μJ/脉冲、445μJ/脉冲、19μJ/脉冲和31μJ/脉冲.","authors":[{"authorName":"涂朝阳","id":"d3ae6ffd-8f45-4a1a-a264-07b56aa7dcb8","originalAuthorName":"涂朝阳"},{"authorName":"李坚富","id":"8ca5f9cb-1f44-4a66-a71b-971e07eb79df","originalAuthorName":"李坚富"},{"authorName":"朱昭捷","id":"2c0a6265-dea2-4c8a-984a-23def8d5cc4a","originalAuthorName":"朱昭捷"},{"authorName":"吴柏昌","id":"350db972-cb93-4d44-b8db-5c717489661f","originalAuthorName":"吴柏昌"},{"authorName":"邱闽旺","id":"97e49228-db4d-4c57-a912-314a2ed931b5","originalAuthorName":"邱闽旺"},{"authorName":"AlainBrenier","id":"60a45188-f4d0-405a-91c9-f6131dcd81c3","originalAuthorName":"AlainBrenier"}],"categoryName":"|","doi":"","fpage":"57","id":"a67a3afd-2315-4caf-970c-9c78fd6de639","issue":"1","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"962279b5-830c-4dd0-b014-170db0163a25","keyword":"熔盐法晶体生长","originalKeyword":"熔盐法晶体生长"},{"id":"a76ed802-7c4c-46d0-83f8-dc7f33f2aebc","keyword":" Nd<SUP><span style=\"color:red\">3</span>+</SUP>:<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>（<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>）<SUB><span style=\"color:red\">4</span></SUB> crystal","originalKeyword":" Nd<SUP>3+</SUP>:GdAl<SUB>3</SUB>（BO<SUB>3</SUB>）<SUB>4</SUB> crystal"},{"id":"61cd4bb4-aac6-41ed-a8c5-ccb78a492749","keyword":" self-frequency changing laser experiment","originalKeyword":" self-frequency changing laser experiment"}],"language":"zh","publisherId":"1000-324X_2003_1_2","title":"自变频激光晶体Nd<SUP><span style=\"color:red\">3</span>+</SUP>:<span style=\"color:red\">GdAl</span><SUB><span style=\"color:red\">3</span></SUB>(<span style=\"color:red\">BO</span><SUB><span style=\"color:red\">3</span></SUB>)<SUB><span style=\"color:red\">4</span></SUB>的研究","volume":"18","year":"2003"},{"abstractinfo":"采用熔盐法生长出尺寸为30mm的Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>优质晶体,进行了吸收光谱和荧光光谱的测定研究,计算得到晶体发射截面为σ1061.9e=2.9×10-19cm2和σ1338nme=5.5×10-20cm2.采用染料激光器作为泵浦源,对晶体进行了自变频激光实验研究,在紫外可调谐(378～382nm)、绿光531nm、蓝光(436～443nm)、红光(669nm)和红外可调谐(1305～1365nm)波段实现了激光输出,输出的最大功率分别为:105μJ/脉冲、119.5μJ/脉冲、445μJ/脉冲、19μJ/脉冲和31μJ/脉冲.","authors":[{"authorName":"涂朝阳","id":"1b7a02bb-e6d8-4474-b284-5927451f1bba","originalAuthorName":"涂朝阳"},{"authorName":"李坚富","id":"78b90e0d-b77c-464c-ba3d-cb04e0e8a0ca","originalAuthorName":"李坚富"},{"authorName":"朱昭捷","id":"1fd7b1d2-6585-45f5-a2b6-8d2b2d26cf34","originalAuthorName":"朱昭捷"},{"authorName":"吴柏昌","id":"8edc7a07-18e9-4f5c-aa1c-71e75e514c4a","originalAuthorName":"吴柏昌"},{"authorName":"邱闽旺","id":"3597a678-5523-4f86-89c2-f44d5126bd73","originalAuthorName":"邱闽旺"},{"authorName":"Alain Brenier","id":"39376d06-99ee-45da-b9b7-cdf8d259a29c","originalAuthorName":"Alain Brenier"}],"doi":"10.3321/j.issn:1000-324X.2003.01.009","fpage":"57","id":"db3e7a0a-bf8a-4889-8933-6810257ae22c","issue":"1","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"3d7aecf3-9149-449d-9767-7eb79d9ec589","keyword":"熔盐法晶体生长","originalKeyword":"熔盐法晶体生长"},{"id":"e8157955-f34e-42b5-b940-350930dabbee","keyword":"Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>晶体","originalKeyword":"Nd3+:GdAl3(BO3)4晶体"},{"id":"d9056707-0f35-4399-8e99-f9344494be0c","keyword":"自变频激光实验","originalKeyword":"自变频激光实验"}],"language":"zh","publisherId":"wjclxb200301009","title":"自变频激光晶体Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>的研究","volume":"18","year":"2003"},{"abstractinfo":"我们用K2Mo<span style=\"color:red\">3O10-B2O3</span>助熔剂生长出尺寸为35 mm的优质Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>激光晶体,测定了偏振的吸收和发射光谱.加工出长度为4.60 mm的激光器件,用染料激光器泵浦,通过晶体的自倍频得到119.5μJ的绿色激光输出,光-光转换效率为4.3%;通过晶体的自和频得到445μJ的蓝色激光输出,光-光转换效率为7.3%.","authors":[{"authorName":"朱昭捷","id":"9f962fd3-5e47-4dee-b1bc-b31cbe4c12ca","originalAuthorName":"朱昭捷"},{"authorName":"李坚富","id":"6acbd13e-53da-406a-8cf2-fd2e6200cdb1","originalAuthorName":"李坚富"},{"authorName":"江爱栋","id":"db392bc4-8de9-409a-bb3c-09eb49dd47e2","originalAuthorName":"江爱栋"},{"authorName":"邱闽旺","id":"7e34c390-d5c3-4c2b-b44f-70c764cbf8e7","originalAuthorName":"邱闽旺"},{"authorName":"涂朝阳","id":"9ba05ded-4416-4645-b83e-a6f3dd2fdead","originalAuthorName":"涂朝阳"}],"doi":"10.3969/j.issn.1007-5461.2001.06.010","fpage":"516","id":"a3666cd5-1f5e-4630-a280-00a724df864c","issue":"6","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"da3f7a87-3451-4ad7-a749-13b5005f3dfe","keyword":"晶体生长","originalKeyword":"晶体生长"},{"id":"4dbea62b-878d-4aef-9837-9f488c056b1b","keyword":"自倍频特性","originalKeyword":"自倍频特性"},{"id":"e9b0f460-7a1f-4b50-983b-02b3da1c336c","keyword":"自和频特性","originalKeyword":"自和频特性"},{"id":"09349980-5002-40b2-86e1-c2773a4ad0f6","keyword":"Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>晶体","originalKeyword":"Nd3+:GdAl3(BO3)4晶体"}],"language":"zh","publisherId":"lzdzxb200106010","title":"Nd<span style=\"color:red\">3</span>+:<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>晶体的蓝绿色激光特性","volume":"18","year":"2001"},{"abstractinfo":"为开发出等离子显示屏用新型红色荧光体,研究了<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>∶Eu,Gd2SiO5∶Eu的紫外和真空紫外发光特性.在147nm激发下<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>∶Eu<span style=\"color:red\">3</span>+呈色坐标为(0.645,0.330)的强红光发射,说明是非常有前途的PDP用红色发光材料.在<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>∶Eu<span style=\"color:red\">3</span>+的激发光谱中,除观察到Eu<span style=\"color:red\">3</span>+的电荷迁移带(峰值位于258nm)外,还观察到峰值位于155nm的宽带.依据硼酸盐的吸收数据将其归属于<span style=\"color:red\">BO3</span>基团的吸收.另外观察到Gd<span style=\"color:red\">3</span>+8S7/2→6I11/2跃迁(274nm)及在真空紫外(158～160nm)激发下,Eu<span style=\"color:red\">3</span>+的红光发射强度随着Eu<span style=\"color:red\">3</span>+浓度的增加而减弱,说明<span style=\"color:red\">BO3</span>基团吸收的能量经Gd<span style=\"color:red\">3</span>+为媒介转移到Eu<span style=\"color:red\">3</span>+.分析Gd2SiO5∶Eu的激发光谱,得到Eu<span style=\"color:red\">3</span>+的电荷迁移带是峰值位于256nm的宽带,峰值位于183nm的宽带可能是Gd<span style=\"color:red\">3</span>+的电荷迁移带.在256nm激发下Gd2SiO5∶Eu<span style=\"color:red\">3</span>+呈强红光发射,但是147nm激发下很弱.这是由于真空紫外激发效率低的原因,其特点可由其晶体结构即激活离子所处的环境解释.","authors":[{"authorName":"王育华","id":"65a43249-f255-4575-80ce-e8d1f8d77401","originalAuthorName":"王育华"},{"authorName":"Endo Tadshi","id":"00648ab6-60e0-404c-922c-8a205a09d8b8","originalAuthorName":"Endo Tadshi"}],"doi":"10.3969/j.issn.1007-2780.2003.05.002","fpage":"325","id":"80c41b5e-397b-46a9-ac15-cf124968b1d0","issue":"5","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示   "},"keywords":[{"id":"0f97989a-00e3-4d52-8e99-79a7de40ed8d","keyword":"等离子显示屏","originalKeyword":"等离子显示屏"},{"id":"bab70898-cb0e-450c-b990-fbd57a120d95","keyword":"<span style=\"color:red\">GdAl3</span>(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">4</span>","originalKeyword":"GdAl3(BO3)4"},{"id":"1513c1e2-6f75-40b0-9d10-38d80f2a5515","keyword":"Gd2SiO5∶Eu","originalKeyword":"Gd2SiO5∶Eu"},{"id":"f4fee2e6-0b29-4c46-95d5-7b064744008e","keyword":"发光体","originalKeyword":"发光体"}],"language":"zh","publisherId":"yjyxs200305002","title":"等离子显示屏(PDP)用新型红色发光体的合成及光学特性","volume":"18","year":"2003"},{"abstractinfo":"采用顶部籽晶法生长出了40 ×10 ×<span style=\"color:red\">3</span> mm<span style=\"color:red\">3</span>和32×10×2mm<span style=\"color:red\">3</span>的非线性光学晶体Cd<span style=\"color:red\">4</span>BiO( <span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>.用XRD粉末衍射和热重-差示扫描量热仪确定了该晶体为同成分熔融晶体,熔点为897℃,在990℃以上开始分解.测量了晶体300 ～ 6500nm的室温透过光谱,结果表明Cd<span style=\"color:red\">4</span> BiO( <span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>晶体在750～2550nm的透过率约为80％,紫外截止波长为395 nm.","authors":[{"authorName":"张文林","id":"0c6cae01-2d39-401d-821b-6e6697c646bc","originalAuthorName":"张文林"},{"authorName":"沈德忠","id":"dc72b5bc-15b7-4121-a7d5-5a922421bf61","originalAuthorName":"沈德忠"}],"doi":"","fpage":"551","id":"bdc88521-7bfe-4932-a7d0-8fdd25f48f11","issue":"3","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"8ca284ef-ed31-4a73-8cb2-33aa4d33c71d","keyword":"顶部籽晶法","originalKeyword":"顶部籽晶法"},{"id":"47fc6e1f-e175-40c5-83b1-054934e61f62","keyword":"非线性光学晶体","originalKeyword":"非线性光学晶体"},{"id":"9d86743c-bb93-4c8d-9d88-b1110ae16228","keyword":"透过率","originalKeyword":"透过率"}],"language":"zh","publisherId":"rgjtxb98201203002","title":"Cd<span style=\"color:red\">4</span>BiO(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>的生长与透过光谱","volume":"41","year":"2012"},{"abstractinfo":"介绍了高质量Ca<span style=\"color:red\">4</span>GdO(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>(GdCOB)、Ca<span style=\"color:red\">4</span>YO(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>(YCOB)晶体的生长,报道了两种晶体空间方向的确定方法,对于该类低对称性非线性光学晶体的实用化具有推动意义.","authors":[{"authorName":"王正平","id":"3bf3dfe5-4276-404e-aafa-814a52580ac1","originalAuthorName":"王正平"},{"authorName":"许心光","id":"621982e3-0833-4858-acad-7c845b81bf84","originalAuthorName":"许心光"},{"authorName":"孙洵","id":"cd1da8dc-0142-4ef9-a837-2abca9e7de27","originalAuthorName":"孙洵"},{"authorName":"王继扬","id":"5dba7746-19e4-4b8d-8cf7-f8eaf7b4bbfd","originalAuthorName":"王继扬"},{"authorName":"邵宗书","id":"12ab60c8-c607-4ca6-aa10-a15f511f4b8a","originalAuthorName":"邵宗书"}],"doi":"10.3321/j.issn:1000-324X.2001.06.027","fpage":"1199","id":"36381529-6d34-498a-b0a1-43da093181b3","issue":"6","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"f93f0c2a-b177-4a02-b642-22b66cba06f5","keyword":"GdCOB晶体","originalKeyword":"GdCOB晶体"},{"id":"1c5e7b62-0ca3-48ba-850f-d4652dd6f709","keyword":"YCOB晶体","originalKeyword":"YCOB晶体"},{"id":"d84966c5-4345-4357-a731-e90dae761230","keyword":"空间方向","originalKeyword":"空间方向"}],"language":"zh","publisherId":"wjclxb200106027","title":"Ca<span style=\"color:red\">4</span>RO(<span style=\"color:red\">BO3</span>)<span style=\"color:red\">3</span>(R=Gd,Y)晶体空间方向的确定","volume":"16","year":"2001"}],"totalpage":7902,"totalrecord":79015}