{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"利用磁控溅射技术,在不同偏压条件下在Si(001)基底上沉积了金属Cr薄膜样品.用同步辐射装置对样品进行了<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span><span style=\"color:red\">反射率</span>测试,采用<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span><span style=\"color:red\">反射率</span><span style=\"color:red\">分析</span>法研究了不同偏压下Cr薄膜密度的变化.发现当偏压小于300V时,偏压对所沉积的薄膜起到紧致的效果,偏压为300V时薄膜密度最大;当偏压大于300V时,薄膜密度减小.另外,为了探究偏压对薄膜表面形貌的影响,用扫描电子显微镜对各样品进行了表面<span style=\"color:red\">分析</span>,发现在偏压较小时薄膜表面较为平整;随着偏压增大,表面呈现界面分明的岛状分布.","authors":[{"authorName":"孙钢杰","id":"134b04d6-8f53-4cfd-a6ce-dc0a0c129d87","originalAuthorName":"孙钢杰"},{"authorName":"伊福廷","id":"7135b74f-559a-4a50-a861-359735cb25d1","originalAuthorName":"伊福廷"},{"authorName":"王焕华","id":"35591178-c6c5-4a7f-b0be-641db0e1e42f","originalAuthorName":"王焕华"},{"authorName":"贾全杰","id":"9ddc2736-5c3c-4858-b54c-460774d3b376","originalAuthorName":"贾全杰"},{"authorName":"张天冲","id":"3012c959-f4ec-4a42-929c-8a8dd99e69c5","originalAuthorName":"张天冲"}],"doi":"10.3969/j.issn.1001-3849.2016.07.001","fpage":"1","id":"c79f655f-886c-4117-9b00-0b6683b11b12","issue":"7","journal":{"abbrevTitle":"DDYJS","coverImgSrc":"journal/img/cover/DDYJS.jpg","id":"20","issnPpub":"1001-3849","publisherId":"DDYJS","title":"电镀与精饰   "},"keywords":[{"id":"5875f204-24f9-481c-8481-5f791b16f0d0","keyword":"<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span><span style=\"color:red\">反射率</span><span style=\"color:red\">分析</span>","originalKeyword":"X-射线反射率分析"},{"id":"70eb9320-0c1d-4def-a1c9-90b92ccf6b9e","keyword":"铬薄膜","originalKeyword":"铬薄膜"},{"id":"7a8d9be7-094f-42cc-b9a6-bd13a1f7c2fc","keyword":"密度","originalKeyword":"密度"},{"id":"c4747398-4128-4c21-8e53-896cbdc94fbb","keyword":"表面形貌","originalKeyword":"表面形貌"},{"id":"bd72bb08-54af-439d-9ed4-cbfbe8e7c822","keyword":"磁控溅射","originalKeyword":"磁控溅射"},{"id":"f8e6e57f-fb85-425e-a7a7-5a2f5e6fc21f","keyword":"偏压","originalKeyword":"偏压"}],"language":"zh","publisherId":"ddjs201607001","title":"磁控溅射偏压对Cr薄膜密度以及表面形貌的影响","volume":"38","year":"2016"},{"abstractinfo":"对实际软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜中普遍存在的主要非理想因素(层厚漂移、界面粗糙度和界面扩散)进行了定量描述基于动力学光学理论,计算了上述非理想因素对软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的掠入射镜向<span style=\"color:red\">反射率</span>的影响结果表明:层厚的随机漂移使<span style=\"color:red\">反射率</span>、尤其是高级<span style=\"color:red\">反射率</span>降低;累积层厚漂移破坏了多层膜的长程有序性,使<span style=\"color:red\">反射</span>峰展宽;界面扩散和界面粗糙度使<span style=\"color:red\">反射率</span>降低,对高级<span style=\"color:red\">反射率</span>的影响更甚,但二者并不破坏多层膜的长程有序性,所以<span style=\"color:red\">反射</span>峰的宽度不变;界面扩散和界面粗糙度对<span style=\"color:red\">反射率</span>影响的机制不同;在界面扩散宽度和界面粗糙度相等的情况下,界面粗糙度使<span style=\"color:red\">反射率</span>下降显著用模拟退火Monte-Carlo方法对Co/C软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜进行了结构评价.该方法能避免复杂的求导运算,在软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的结构评价中具有较强的实用性.","authors":[{"authorName":"白海力","id":"17544cc9-6e77-463b-af00-f0cf53ea53bb","originalAuthorName":"白海力"},{"authorName":"何忠杰","id":"73225de8-90f2-4eb5-9b9b-11271eed86ab","originalAuthorName":"何忠杰"},{"authorName":"田仁玉","id":"b4f2b44a-96e0-4667-8f77-dafa201d96d7","originalAuthorName":"田仁玉"},{"authorName":"姜恩永","id":"29329c40-1d9b-4683-b5b4-b44874c147dc","originalAuthorName":"姜恩永"}],"categoryName":"|","doi":"","fpage":"121","id":"5edd6eb6-1f6a-4558-9010-cd688021a80b","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"b4557555-0eff-452e-849e-db5579dc49b2","keyword":"软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜","originalKeyword":"软X射线光学多层膜"},{"id":"a32f6e68-3de7-444c-bf25-4c81dfa13f18","keyword":"null","originalKeyword":"null"},{"id":"9cfeb777-07b7-4653-9a6a-281e8b9d0791","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"0412-1961_2001_2_11","title":"非理想软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的掠入射镜向<span style=\"color:red\">反射率</span>","volume":"37","year":"2001"},{"abstractinfo":"对实际软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜中普遍存在的主要非理想因素(层厚漂移、界面粗糙度和界面扩散)进行了定量描述基于动力学光学理论,计算了上述非理想因素对软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的掠入射镜向<span style=\"color:red\">反射率</span>的影响结果表明:层厚的随机漂移使<span style=\"color:red\">反射率</span>、尤其是高级<span style=\"color:red\">反射率</span>降低;累积层厚漂移破坏了多层膜的长程有序性,使<span style=\"color:red\">反射</span>峰展宽;界面扩散和界面粗糙度使<span style=\"color:red\">反射率</span>降低,对高级<span style=\"color:red\">反射率</span>的影响更甚,但二者并不破坏多层膜的长程有序性,所以<span style=\"color:red\">反射</span>峰的宽度不变;界面扩散和界面粗糙度对<span style=\"color:red\">反射率</span>影响的机制不同;在界面扩散宽度和界面粗糙度相等的情况下,界面粗糙度使<span style=\"color:red\">反射率</span>下降显著用模拟退火Monte-Carlo方法对Co/C软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜进行了结构评价.该方法能避免复杂的求导运算,在软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的结构评价中具有较强的实用性","authors":[{"authorName":"白海力","id":"3a716b89-3c9c-472a-b49c-47b5b7f69cbb","originalAuthorName":"白海力"},{"authorName":"何忠杰","id":"a54086b6-2c66-4a3d-ab10-d12bc150cde6","originalAuthorName":"何忠杰"},{"authorName":"田仁玉","id":"e7fc81c4-4148-454f-9859-b548b4ba6e0c","originalAuthorName":"田仁玉"},{"authorName":"姜恩永","id":"67beb97c-a7f5-47c2-a59a-431f2b348048","originalAuthorName":"姜恩永"}],"doi":"10.3321/j.issn:0412-1961.2001.02.003","fpage":"121","id":"82004c2b-841f-4732-84af-402fdb5688ce","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"4d73aefe-a292-4f0f-b350-28b284d85d06","keyword":"软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜","originalKeyword":"软X射线光学多层膜"},{"id":"00e03635-70d2-4d62-bd81-5a1c5f2680e6","keyword":"层厚漂移","originalKeyword":"层厚漂移"},{"id":"a6abd238-23a2-4fb5-8dec-7d8db8ddde61","keyword":"界面粗糙度","originalKeyword":"界面粗糙度"},{"id":"b92667ca-5f1c-4426-98e8-697c4e31b265","keyword":"界面扩散","originalKeyword":"界面扩散"},{"id":"cf41fb6e-2245-4b17-95e6-bc04cb976a96","keyword":"掠入射镜向<span style=\"color:red\">反射率</span>","originalKeyword":"掠入射镜向反射率"},{"id":"1e920bca-524a-4b3e-b4f5-f75f1ce7a006","keyword":"模拟退火Monte-Carlo方法","originalKeyword":"模拟退火Monte-Carlo方法"}],"language":"zh","publisherId":"jsxb200102003","title":"非理想软<span style=\"color:red\">X</span><span style=\"color:red\">射线</span>光学多层膜的掠入射镜向<span style=\"color:red\">反射率</span>","volume":"37","year":"2001"},{"abstractinfo":"采用化学镀镍和聚苯胺包覆分别对碳纤维布进行表面改性。表征了不同方法改性前后碳纤维布的表观形貌和导电性，并采用弓形法对碳纤维布在<span style=\"color:red\">X</span>波段的雷达<span style=\"color:red\">反射率</span>进行测试。结果表明，未改性、镀镍和聚苯胺包覆碳纤维布的电阻分别为24.2、22.6和60.6?。频率较低时，镀镍碳纤维布的雷达<span style=\"color:red\">反射率</span>低于未改性碳纤维布；在8~12 GHz全频段，前者的平均<span style=\"color:red\">反射率</span>比后者高22.35%。聚苯胺包覆碳纤维布在8~12 GHz全频段内的雷达<span style=\"color:red\">反射率</span>均小于改性前的碳纤维布，其平均<span style=\"color:red\">反射率</span>降低了104.71%。","authors":[{"authorName":"过凯","id":"5e932b1e-2543-4ea1-a589-52064ff82404","originalAuthorName":"过凯"},{"authorName":"关华","id":"c52024bd-e433-41ce-9e69-b03ec61cd0e0","originalAuthorName":"关华"},{"authorName":"宋东明","id":"2343430f-7390-4727-9adf-95e99fed6b80","originalAuthorName":"宋东明"}],"doi":"","fpage":"189","id":"2a8513a1-010f-4e7d-9dbd-f0e14175e954","issue":"5","journal":{"abbrevTitle":"DDYTS","coverImgSrc":"journal/img/cover/DDYTS.jpg","id":"21","issnPpub":"1004-227X","publisherId":"DDYTS","title":"电镀与涂饰   "},"keywords":[{"id":"221b9f1b-44f3-462a-b519-27e3617b04d6","keyword":"碳纤维布","originalKeyword":"碳纤维布"},{"id":"904cb336-dfdd-4518-88ee-077ae6c12f3c","keyword":"化学镀镍","originalKeyword":"化学镀镍"},{"id":"c5ba1f9f-300b-4e0d-bacc-c76b5729780c","keyword":"聚苯胺包覆","originalKeyword":"聚苯胺包覆"},{"id":"8948e033-579d-4543-a43b-4cc7b5db1b77","keyword":"雷达波<span style=\"color:red\">反射率</span>","originalKeyword":"雷达波反射率"},{"id":"932b3bbd-bed9-4b53-8ae2-bf570f69b323","keyword":"弓形法","originalKeyword":"弓形法"}],"language":"zh","publisherId":"ddyts201405002","title":"不同改性方法对碳纤维布<span style=\"color:red\">X</span>波段雷达<span style=\"color:red\">反射率</span>的影响","volume":"","year":"2014"},{"abstractinfo":"针对OMIS I机载成像光谱数据,通过6S辐射传输码模拟计算和相应理论<span style=\"color:red\">分析</span>,讨论了观测角变化对传感器入瞳处辐射亮度的影响和由此引起的<span style=\"color:red\">反射率</span>反演误差.结果表明:在太阳<span style=\"color:red\">反射</span>波段,观测角的影响有很强的波段特性,大气散射作用较强的短波长波段与大气气体强吸收波段是这种影响的敏感波段;地面目标亮度不同,这种影响也是不同的,对低<span style=\"color:red\">反射率</span>目标影响较大,而对高<span style=\"color:red\">反射率</span>目标影响甚微;另外遥感器飞行高度也是决定这种影响情况的重要因素.","authors":[{"authorName":"杨本永","id":"11192c0a-ffa9-4df9-87fd-3956925f64fb","originalAuthorName":"杨本永"},{"authorName":"方勇华","id":"fff133e3-8cec-40c4-947a-d89c1b070fa7","originalAuthorName":"方勇华"},{"authorName":"孙桂玲","id":"ab3302e7-b702-48cc-a290-c75b08d664bb","originalAuthorName":"孙桂玲"}],"doi":"10.3969/j.issn.1007-5461.2005.04.037","fpage":"667","id":"8c99c6e4-adfc-4973-9050-34c2788210b6","issue":"4","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":"6d6792e6-554b-43d9-8f97-92e51d88690b","keyword":"遥感","originalKeyword":"遥感"},{"id":"90b35742-8d17-4a1a-a773-3ff1be10dbbe","keyword":"成像光谱数据","originalKeyword":"成像光谱数据"},{"id":"576ab8ca-a3fa-4870-91e7-90d77ab58a90","keyword":"模拟计算","originalKeyword":"模拟计算"},{"id":"7e7fbca2-4dcc-41a7-9f68-c22d4b3ece68","keyword":"观测天顶角","originalKeyword":"观测天顶角"},{"id":"a9a7762a-3e23-4377-be7c-49a424e6dc6e","keyword":"<span style=\"color:red\">反射率</span>反演","originalKeyword":"反射率反演"}],"language":"zh","publisherId":"lzdzxb200504037","title":"成像光谱<span style=\"color:red\">反射率</span>反演中观测角影响的<span style=\"color:red\">分析</span>","volume":"22","year":"2005"},{"abstractinfo":"根据边界衍射波理论,对<span style=\"color:red\">反射率</span>呈高斯类函数(n=2)、抛物类函数(n=1, 2) 以及线性坡度递减分布的腔镜的边界衍射光场作了<span style=\"color:red\">分析</span>和比较,结果表明了<span style=\"color:red\">反射率</span>呈高斯类函数分布的腔镜能更有效地减弱边界衍射光场,获得高质量的准几何光学近似的基模光场。","authors":[{"authorName":"葛传文","id":"3f88fbfd-14e8-4fa1-abde-e2ccc6540027","originalAuthorName":"葛传文"},{"authorName":"张为俊","id":"82811957-7a8c-4e76-a75b-bb7cd3c654c6","originalAuthorName":"张为俊"},{"authorName":"王沛","id":"79b2d18b-8766-4123-a990-e594b7eeaea2","originalAuthorName":"王沛"},{"authorName":"袁仁民","id":"85c2c758-d2ae-462b-8a76-f4dd3227b2d4","originalAuthorName":"袁仁民"},{"authorName":"聂劲松","id":"1be62983-4953-4225-87d2-35503a5b95ba","originalAuthorName":"聂劲松"},{"authorName":"程平","id":"61ae6aa0-d4c9-4691-bb1a-ad58a1790339","originalAuthorName":"程平"}],"doi":"10.3969/j.issn.1007-5461.2000.02.002","fpage":"108","id":"7f3ad0fb-06eb-4523-a35b-ef39e1bed083","issue":"2","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":"57c7f9f6-02cd-40d7-9ec7-bed2b19f0c84","keyword":"边界衍射光场","originalKeyword":"边界衍射光场"},{"id":"920b3e7b-779e-4440-8e32-0420df7c0024","keyword":"变<span style=\"color:red\">反射率</span>腔镜","originalKeyword":"变反射率腔镜"},{"id":"2da38a12-3ab9-4375-a8dd-8a7ee57773e6","keyword":"高斯类函数分布","originalKeyword":"高斯类函数分布"}],"language":"zh","publisherId":"lzdzxb200002002","title":"几种变<span style=\"color:red\">反射率</span>腔镜边界衍射光场强度的理论<span style=\"color:red\">分析</span>与比较","volume":"17","year":"2000"},{"abstractinfo":"采用传统的节能减排的方法来控制地球温室效应需要在全世界范围内进行协调,这是一项十分艰难的工作,若能采用<span style=\"color:red\">反射</span>板等将太阳能量向太空<span style=\"color:red\">反射</span>,则是人类采用技术手段来主动控制温室效应,执行起来要容易、可行得多.本文以美国杜邦油漆为例,研究了在金属基底上喷涂白漆涂层对太阳能量的光谱<span style=\"color:red\">反射率</span>,研究显示,杜邦白漆涂层在太阳辐射的峰值波段具有很大的<span style=\"color:red\">反射率</span>,达到了90％以上,在未考虑大气作用的情况下,白油漆对太阳能量的平均<span style=\"color:red\">反射率</span>达到了71.6％,杜邦其它颜色漆的<span style=\"color:red\">反射率</span>均没有白油漆大.","authors":[{"authorName":"罗剑峰","id":"4a5b1232-fdc6-4ae2-ab3e-16f9871613eb","originalAuthorName":"罗剑峰"},{"authorName":"邓邛","id":"c6135637-083e-4e36-84b4-03cc44799ff5","originalAuthorName":"邓邛"},{"authorName":"杨俊波","id":"55551c28-73d4-4db5-9c95-89292de4b81d","originalAuthorName":"杨俊波"},{"authorName":"易洪亮","id":"cbff8002-dcc1-4b2f-a2aa-1f72fa114443","originalAuthorName":"易洪亮"},{"authorName":"谈和平","id":"9502f0b5-712d-46f0-84bb-4d5ebacc59a9","originalAuthorName":"谈和平"}],"doi":"","fpage":"2467","id":"b3b3bc24-3744-447a-9fbd-4e0267253688","issue":"11","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"f9335ea5-0695-41e4-8348-d12f59a7c9ad","keyword":"温室效应","originalKeyword":"温室效应"},{"id":"eb7d2d35-df4f-4db3-9ddb-7b749fb69097","keyword":"光谱<span style=\"color:red\">反射率</span>","originalKeyword":"光谱反射率"},{"id":"d5dc74b4-7fe3-4b7d-92a4-865e02dd8dfe","keyword":"太阳辐射","originalKeyword":"太阳辐射"},{"id":"848fc78e-e0c1-4ca4-9557-d9be7710ca8b","keyword":"白油漆涂层","originalKeyword":"白油漆涂层"},{"id":"42bc53e1-e94f-4870-abf4-f99c2f5d0fa9","keyword":"杜邦漆","originalKeyword":"杜邦漆"}],"language":"zh","publisherId":"gcrwlxb201511033","title":"金属基底白漆涂层的光谱<span style=\"color:red\">反射率</span>","volume":"36","year":"2015"},{"abstractinfo":"运用<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>衍射<span style=\"color:red\">分析</span>技术研究了不同成分铜基形状记忆合金淬火态马氏体结构、马氏体状态非等温时效过程中结构的变化规律、母相状态时效和连续变形过程中马氏体及母相结构的变化规律以及热循环过程中马氏体结构的变化情况.","authors":[{"authorName":"李周","id":"2982865b-8087-4ef5-b9f2-68744152a4b7","originalAuthorName":"李周"},{"authorName":"郭明星","id":"1be4197f-4daf-45f2-a3f6-7c2df157149a","originalAuthorName":"郭明星"},{"authorName":"曹玲飞","id":"ee9dbb3b-803b-4e5a-ba0f-4fbc4b81f5d7","originalAuthorName":"曹玲飞"}],"doi":"10.3969/j.issn.1005-8192.2004.04.004","fpage":"14","id":"4636a1fd-6ed7-4f4a-9864-c7ca026b38a4","issue":"4","journal":{"abbrevTitle":"JSGNCL","coverImgSrc":"journal/img/cover/JSGNCL.jpg","id":"46","issnPpub":"1005-8192","publisherId":"JSGNCL","title":"金属功能材料"},"keywords":[{"id":"1425bb21-6101-4391-a580-1cc01c2f37d9","keyword":"铜基形状记忆合金","originalKeyword":"铜基形状记忆合金"},{"id":"6dfccfc0-2f4a-4531-ba8c-333cd001c8f3","keyword":"<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>衍射","originalKeyword":"X-射线衍射"},{"id":"ff03dcec-f5c5-44ca-8485-feca51df7fa7","keyword":"马氏体","originalKeyword":"马氏体"}],"language":"zh","publisherId":"jsgncl200404004","title":"铜基形状记忆合金研究中<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>衍射<span style=\"color:red\">分析</span>技术的应用","volume":"11","year":"2004"},{"abstractinfo":"太阳热<span style=\"color:red\">反射</span>涂料是一种可以降低太阳辐射引起升温的节能型涂料.通过对美国军标太阳热<span style=\"color:red\">反射</span>涂层<span style=\"color:red\">反射率</span>测试装置和方法的改进,测试了不同太阳热<span style=\"color:red\">反射</span>涂层的热<span style=\"color:red\">反射率</span>,建立了相应的数学模型并进行可靠性<span style=\"color:red\">分析</span>.该模型可用于不同涂层太阳热<span style=\"color:red\">反射率</span>相对值的比较.通过带积分球的紫外-可见-红外分光光度计的测试数据和模拟储油罐在实际大气环境之下的温度变化曲线,验证了改进方法和数学模型的正确性.基于此方法和模型研制的新型太阳热<span style=\"color:red\">反射</span>涂料,在200～2600nm波段范围内的<span style=\"color:red\">反射率</span>明显优于银粉漆和常规白色涂料,热<span style=\"color:red\">反射</span>降温效果显著.","authors":[{"authorName":"殷燕子","id":"eb93c215-2d29-48ef-b783-7f402cd4f918","originalAuthorName":"殷燕子"},{"authorName":"林安","id":"3ffac0e5-4cc8-4cc8-9731-4a942e1e5590","originalAuthorName":"林安"},{"authorName":"刘秀生","id":"c145f9cd-2108-48ee-acc0-4d901c1ae8d6","originalAuthorName":"刘秀生"},{"authorName":"程学群","id":"408e095a-d764-48b5-b61a-6dbbdc9d5644","originalAuthorName":"程学群"}],"doi":"10.3969/j.issn.1001-1560.2004.05.003","fpage":"8","id":"e7cace9a-2f23-4b1d-a82f-5318d9a66e24","issue":"5","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"a60ad1c9-1707-4d02-8a41-f387a94b4780","keyword":"太阳热<span style=\"color:red\">反射</span>涂料","originalKeyword":"太阳热反射涂料"},{"id":"4b569589-c931-467f-b938-d02b9b01c67a","keyword":"<span style=\"color:red\">反射率</span>检测方法","originalKeyword":"反射率检测方法"},{"id":"6d312e33-d9a0-46cf-b9c6-716a71fbb234","keyword":"数学模型","originalKeyword":"数学模型"}],"language":"zh","publisherId":"clbh200405003","title":"太阳热<span style=\"color:red\">反射</span>涂料的<span style=\"color:red\">反射率</span>检测方法研究及其数学模型","volume":"37","year":"2004"},{"abstractinfo":"本文介绍了用偏硼酸锂(33%)和四硼酸锂(67%)混合助熔剂熔融制样,加补钴粉做内标,采用<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>荧光光谱法定量测定铁矿石中的TFe,SiO2,CaO,MgO,Al2O3,P,S含量,经大量实践数据证明,完全符合误差要求,精密度高,准确度可靠,不仅大大缩短了<span style=\"color:red\">分析</span>时间,提高了工作效率,而且降低了劳动强度.","authors":[{"authorName":"肖文忠","id":"44b3697c-bac8-4200-ad0a-8c50efb5c982","originalAuthorName":"肖文忠"},{"authorName":"苏峥","id":"b225c29a-fdc0-4432-b385-908e99057a69","originalAuthorName":"苏峥"},{"authorName":"马建平","id":"65632b58-3d32-4704-811e-6ce4451f92c8","originalAuthorName":"马建平"},{"authorName":"刘尚英","id":"84734798-bbe7-42f9-a8b3-de972be17bab","originalAuthorName":"刘尚英"}],"doi":"10.3969/j.issn.1000-7571.2004.z1.068","fpage":"232","id":"8bd7e412-cbf5-4cf8-aac3-e32ec58731d8","issue":"z1","journal":{"abbrevTitle":"YJFX","coverImgSrc":"journal/img/cover/YJFX.jpg","id":"71","issnPpub":"1000-7571","publisherId":"YJFX","title":"冶金分析   "},"keywords":[{"id":"38b2f6b5-4f8c-4742-bb8b-3ed95421e837","keyword":"<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>荧光光谱","originalKeyword":"X-射线荧光光谱"},{"id":"177e23a0-d075-46ed-8b6c-fa61f91df231","keyword":"铁矿石","originalKeyword":"铁矿石"},{"id":"caa4faef-f47a-4ce2-a563-c6481e289963","keyword":"熔融法","originalKeyword":"熔融法"}],"language":"zh","publisherId":"yjfx2004z1068","title":"利用<span style=\"color:red\">X-</span><span style=\"color:red\">射线</span>荧光光谱仪<span style=\"color:red\">分析</span>铁矿石中若干元素","volume":"24","year":"2004"}],"totalpage":11871,"totalrecord":118710}