{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"基于第一性原理GGA+U方法研究了Zn1-xCdxO合金的品格常数以及自发极化随Cd组分x的变化关系,其中极化特性的计算采用Berry-phase方法,同时计算了禁带宽度随Cd组分x的变化关系,并得到了能隙弯曲参数0.69.此外,通过计算宏观平均静电势的方法得到了(5 +3)Cd0.25Cd0.750/ZnO超晶格界面处的价带偏差为0.13 eV,导带偏差与价带偏差的比值为4/13,并且Zn1-xCdxO/ZnO界面两侧能带呈现Ⅰ型排列,这些研究结果将对Zn1-xCdxO/ZnO界面二维电子气的设计与优化起到重要作用.","authors":[{"authorName":"吴孔平","id":"4ef3d846-e124-4ea8-838e-c3803ea07c06","originalAuthorName":"吴孔平"},{"authorName":"慈能达","id":"93ab0e6e-81ed-4e7a-9822-1ec752328e67","originalAuthorName":"慈能达"},{"authorName":"汤琨","id":"9e2457ef-abb2-4c85-aac8-f6633c426e7d","originalAuthorName":"汤琨"},{"authorName":"叶建东","id":"b7385c4c-8471-4bde-85ae-b3b597fe9791","originalAuthorName":"叶建东"},{"authorName":"朱顺明","id":"ec3f356d-0e96-42ec-accc-0963ba851e31","originalAuthorName":"朱顺明"},{"authorName":"顾书林","id":"4ceb80f2-036b-45ca-ae52-606df94986c1","originalAuthorName":"顾书林"}],"doi":"","fpage":"2577","id":"cfbcf82d-d675-4278-8966-856a491e4239","issue":"9","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":"8028d678-70fd-498b-bbdb-80a98ea542c0","keyword":"自发极化","originalKeyword":"自发极化"},{"id":"e88c5d1d-262c-4a18-83c9-28a0f8592fd2","keyword":"静电势平均","originalKeyword":"静电势平均"},{"id":"b4c772da-1555-44bf-956d-9d24759dfdc1","keyword":"能带偏差","originalKeyword":"能带偏差"},{"id":"2fa7922d-ded3-4566-b2c5-b0dd9b2e2fa5","keyword":"锌镉氧合金","originalKeyword":"锌镉氧合金"}],"language":"zh","publisherId":"rgjtxb98201509046","title":"Cd对纤锌矿ZnO极化特性的影响以及Zn0.75Cd0.25O/ZnO界面能带偏差的第一性原理研究","volume":"44","year":"2015"},{"abstractinfo":"本文基于Anderson s-d混合模型和Falicov s-d库仑互作用模型,利用格林函数方法,得到局域态电子占有平均值的自洽方程,定量地分析在给定不同的参数下,局域态电子占有数平均值和局域磁矩,研究了稀磁合金的s-d混合效应和s-d库仑互作用效应对热电势的影响.","authors":[{"authorName":"陈丽","id":"6533f54d-253a-4699-8261-8632208c01c2","originalAuthorName":"陈丽"}],"doi":"10.3969/j.issn.1000-3258.2002.02.013","fpage":"137","id":"e63be0d9-1fcf-4a4a-b485-1a81e233f30a","issue":"2","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报 "},"keywords":[{"id":"0b0b21a6-d789-473d-b9e7-f2dd2150e9fe","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"dwwlxb200202013","title":"稀磁合金的局域磁矩与热电势","volume":"24","year":"2002"},{"abstractinfo":"研究了冷轧IF钢板镀锌前后的热电势(TEP)特性。试 验结果表明:镀锌退火后,钢板基体发生再结晶导致TEP值升高,而镀层的形成导致TE P值下降,基体的再结晶起主导作用。并且,TEP值存在各向异性,这与钢板的织构有关 。","authors":[{"authorName":"章跃","id":"2e3efe97-779c-4883-8684-cede7056ef35","originalAuthorName":"章跃"},{"authorName":"","id":"61aa82bd-95e7-431b-a2c4-60b93d25b356","originalAuthorName":""},{"authorName":"","id":"748d62d7-9b7b-4c58-937c-fbbfc32a7809","originalAuthorName":""}],"doi":"10.3969/j.issn.1000-3738.2001.02.010","fpage":"32","id":"1d766474-676c-46f4-bbc0-51ba1f305247","issue":"2","journal":{"abbrevTitle":"JXGCCL","coverImgSrc":"journal/img/cover/JXGCCL.jpg","id":"45","issnPpub":"1000-3738","publisherId":"JXGCCL","title":"机械工程材料"},"keywords":[{"id":"8ea45eec-14dc-4af6-b0a8-466c3988fc00","keyword":"镀锌","originalKeyword":"镀锌"},{"id":"4d4291f6-1112-400d-b653-18c44cc075a0","keyword":"热电势","originalKeyword":"热电势"},{"id":"6d481d4a-808c-4ed8-8d85-858ec9553e2e","keyword":"IF钢板","originalKeyword":"IF钢板"},{"id":"8d58c183-bb3f-42cb-b79e-1d58fb4d1213","keyword":"织构","originalKeyword":"织构"},{"id":"1dbd074e-f875-4341-b3bc-d01fb5cf5063","keyword":"各向异性","originalKeyword":"各向异性"}],"language":"zh","publisherId":"jxgccl200102010","title":"IF钢板镀锌前后热电势的测定","volume":"25","year":"2001"},{"abstractinfo":"高温电阻测量通常采用直流补偿法完成,在具体操作(数据处理)中,普遍取工作电流正、反向过程中测得的电位差值的绝对值数据平均值作为测量结果简称“绝对值法”。实践证明,传统方法在寄生温差电势大的情况下,将导致错误的结果;从理论、实践两方面进行了分析,提出的“代数平均值处理法”;简称“代数值法”,为高温电阻检测方法的重要改进。","authors":[{"authorName":"李丽敏,牛宏凯,李昕","id":"015e6702-1e64-4bcd-8f1d-a898f2541c5d","originalAuthorName":"李丽敏,牛宏凯,李昕"}],"categoryName":"|","doi":"","fpage":"37","id":"ce93a936-0537-46d7-abba-77d28d078a6a","issue":"2","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"edefc78f-e7ec-4a65-b580-03b3abaec1ae","keyword":"高温电阻","originalKeyword":"高温电阻"},{"id":"a623484d-cf08-455d-9bed-ba468935f4d7","keyword":"parasitic potential","originalKeyword":"parasitic potential"},{"id":"e6f83094-500f-411a-bfb5-8b7e83383207","keyword":"compensation method.","originalKeyword":"compensation method."}],"language":"zh","publisherId":"1001-0777_2011_2_2","title":"寄生电势对高温电阻检测影响的研究","volume":"29","year":"2011"},{"abstractinfo":"高温电阻测量通常采用直流补偿法完成.在具体操作(数据处理)中,普遍取工作电流正、反向过程中测得的电位差值的绝对值数据平均值作为测量结果简称\"绝对值法\".实践证明,传统方法在寄生温差电势大的情况下,将导致错误的结果;从理论、实践两方面进行了分析,提出的\"代数平均值处理法\";简称\"代数值法\",为高温电阻检测方法的莺要改进.","authors":[{"authorName":"李丽敏","id":"bb0aaa32-972b-43ea-82be-f3b376b23804","originalAuthorName":"李丽敏"},{"authorName":"牛宏凯","id":"81376fcc-10dd-4702-975a-b286233eb945","originalAuthorName":"牛宏凯"},{"authorName":"李昕","id":"a030fbf2-99b0-4027-a72a-56c0aad2671b","originalAuthorName":"李昕"}],"doi":"","fpage":"37","id":"e9d33031-f37b-4828-ae25-12d7714c0e86","issue":"2","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"a81df7f9-79c1-47c5-afa6-a0f053b37987","keyword":"高温电阻","originalKeyword":"高温电阻"},{"id":"964dad33-1a3d-4247-9c83-c7aa81bd0648","keyword":"寄生电势","originalKeyword":"寄生电势"},{"id":"235a75e9-79f8-4588-b30b-9f6cf3eff39e","keyword":"补偿法","originalKeyword":"补偿法"}],"language":"zh","publisherId":"wlcs201102010","title":"寄生电势对高温电阻检测影响的研究","volume":"29","year":"2011"},{"abstractinfo":"采用动电势扫描法测定了不同体系中碳钢发生点蚀的临界电势Eb.结果表明:当Cl-浓度<0.01 mol/L时,随Cl-浓度增加,临界电势负移并与Cl-浓度成线性关系;pH值在7~11之间,随pH值增加,临界电势正移并与pH值成线性关系;随温度增加,临界电势负移并与温度成线性关系.","authors":[{"authorName":"谷宁","id":"41fe6ee4-39de-48d6-bce8-49e4ee1df553","originalAuthorName":"谷宁"},{"authorName":"李春梅","id":"ac910de9-c2fd-4a86-a684-52821e47e158","originalAuthorName":"李春梅"}],"doi":"10.3969/j.issn.1001-1560.2002.07.008","fpage":"20","id":"13dfb17b-9941-4966-8a34-19687993559b","issue":"7","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"2f3e3799-c5a1-429a-ba72-dd788cc58634","keyword":"碳钢","originalKeyword":"碳钢"},{"id":"08c3dfa2-1472-40ad-9488-3a3636f93bf1","keyword":"点蚀临界电势","originalKeyword":"点蚀临界电势"},{"id":"015d70a8-49cd-43ab-8a77-2acd7e497a96","keyword":"阳极极化曲线","originalKeyword":"阳极极化曲线"}],"language":"zh","publisherId":"clbh200207008","title":"环境因素对碳钢点蚀临界电势的影响","volume":"35","year":"2002"},{"abstractinfo":"根据化学势绘制了室温下在55%LiBr溶液中CuBr-H2O体系的铜的电势-pH图和腐蚀-免蚀-钝化条件图.结果表明,水溶液中Br-离子浓度增大后,Cu2O的稳定存在区域明显减小,CuBr的生成电势负移,溶解电势正移,且其稳定存在区域明显拓宽,导致了铜的免蚀和钝化区域的缩小,腐蚀加剧.电势-pH图的建立对研究高浓度LiBr溶液中铜及其合金的腐蚀行为有一定的参考价值.\n\n","authors":[{"authorName":"梁成浩","id":"c3c98491-ec18-46fb-8bed-795528ea74e4","originalAuthorName":"梁成浩"},{"authorName":"黄乃宝","id":"c2964c20-ff1a-4072-be92-e8a05500c8a1","originalAuthorName":"黄乃宝"},{"authorName":"扈显琦","id":"9620ee11-4d4b-4421-b57a-6f70734dd8a5","originalAuthorName":"扈显琦"}],"categoryName":"|","doi":"","fpage":"157","id":"bd841e4b-17f7-47a2-a07d-703761c7924b","issue":"3","journal":{"abbrevTitle":"FSXB","coverImgSrc":"journal/img/cover/腐蚀学报封面.jpg","id":"24","issnPpub":"2667-2669","publisherId":"FSXB","title":"腐蚀学报(英文)"},"keywords":[{"id":"1a083a29-0af3-4e48-82be-e62892b2a4f5","keyword":"铜","originalKeyword":"铜"},{"id":"78e17670-2882-4e3d-a062-1648a43987a9","keyword":"null","originalKeyword":"null"},{"id":"5e5dbd04-3318-4870-8180-08470fcf849b","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"1002-6495_2006_3_6","title":"铜在55%LiBr溶液中的电势-pH图","volume":"18","year":"2006"},{"abstractinfo":"根据化学势绘制了室温下在55%LiBr溶液中Cu-Br--H2O体系的铜的电势-pH图和腐蚀-免蚀-钝化条件图.结果表明,水溶液中Br-离子浓度增大后,Cu2O的稳定存在区域明显减小,CuBr的生成电势负移,溶解电势正移,且其稳定存在区域明显拓宽,导致了铜的免蚀和钝化区域的缩小,腐蚀加剧.电势-pH图的建立对研究高浓度LiBr溶液中铜及其合金的腐蚀行为有一定的参考价值.","authors":[{"authorName":"梁成浩","id":"08a24bc1-3ac6-4342-8777-bae4e4839050","originalAuthorName":"梁成浩"},{"authorName":"黄乃宝","id":"55dd15c2-e767-4fda-a321-c90cb4ea0140","originalAuthorName":"黄乃宝"},{"authorName":"扈显琦","id":"49d3bafe-55ca-4997-aeaf-9a8a7b275bad","originalAuthorName":"扈显琦"}],"doi":"10.3969/j.issn.1002-6495.2006.03.001","fpage":"157","id":"4a0be248-4519-4888-bf4e-381e1e94f530","issue":"3","journal":{"abbrevTitle":"FSXB","coverImgSrc":"journal/img/cover/腐蚀学报封面.jpg","id":"24","issnPpub":"2667-2669","publisherId":"FSXB","title":"腐蚀学报(英文)"},"keywords":[{"id":"f5832eb2-4771-4e1c-b0a3-b3434fc1f066","keyword":"铜","originalKeyword":"铜"},{"id":"37824957-dc6a-425f-b95f-95fa7ccf7484","keyword":"溴化锂","originalKeyword":"溴化锂"},{"id":"c797c15f-e9cb-4a4d-9d54-74fdfb64d51c","keyword":"电势-pH图","originalKeyword":"电势-pH图"}],"language":"zh","publisherId":"fskxyfhjs200603001","title":"铜在55%LiBr溶液中的电势-pH图","volume":"18","year":"2006"},{"abstractinfo":"基于Gross-Pitaevskii(G-P)平均场能量泛函,运用分步傅里叶方法研究了可控的无序光斑电势中弱相互作用玻色凝聚气体的安德森局域化.研究结果表明:1)类高斯指数型的试探函数在变分分析过程中取得了预期效果;2)无序度η为1,相互作用强度κ为0.1的条件下,当电势特征强度Vs大于0.6倍化学势(0.6μ)时,凝聚气体在演化过程中能够保持稳定的局域化状态;3)较大的原子间相互作用(κ>5)对安德森局域化的稳定性产生不利影响; 4)Vs为0.6 μ,κ为0.1的条件下,光斑电势的无序度η越大,凝聚气体的安德森局域化越明显.","authors":[{"authorName":"陈传书","id":"0379e818-61c1-4c30-a3e6-c740f71c6af0","originalAuthorName":"陈传书"},{"authorName":"徐志君","id":"946658c9-78b7-47e1-bae6-0402edca53c5","originalAuthorName":"徐志君"}],"doi":"10.3969/j.issn.1007-5461.2014.05.010","fpage":"576","id":"550df2da-9c74-4ea7-8062-46e22f782fe3","issue":"5","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":"8eef3c60-4cbd-429d-a66e-1736d0721d58","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"2624a821-c2db-435e-be24-99406a23d854","keyword":"安德森局域化","originalKeyword":"安德森局域化"},{"id":"230e8a7a-a788-4d1d-9b12-4a6d26067261","keyword":"Gross-Pitaevskii方程","originalKeyword":"Gross-Pitaevskii方程"},{"id":"0169f34b-e0f0-4c61-9c8c-32ae06ab68eb","keyword":"无序光斑电势","originalKeyword":"无序光斑电势"},{"id":"ff883847-ff85-4ffe-8f30-801d796e9604","keyword":"玻色凝聚气体","originalKeyword":"玻色凝聚气体"}],"language":"zh","publisherId":"lzdzxb201405010","title":"无序光斑电势中玻色凝聚气体的安德森局域化","volume":"31","year":"2014"},{"abstractinfo":"测试了 MESFET工艺条件下制作的霍尔片的基本性能.对设计出的 GaAs集成霍尔元件进 行了不等位电势的测试,采用霍尔元件并联和自旋电流的方法对 GaAs方形霍尔元件的不等位电 势进行了静态和动态调制消除.实验结果表明 GaAs霍尔元件的不等位电势引起的偏差可以控制 在可以忽略的范围内.","authors":[{"authorName":"冯明","id":"24062db3-7338-45b8-81cd-f283779c9f42","originalAuthorName":"冯明"},{"authorName":"夏冠群","id":"f470c648-4c11-4f53-8786-8127cc573aee","originalAuthorName":"夏冠群"},{"authorName":"胡少坚","id":"b72626fd-60ee-4827-b340-1c2167a46558","originalAuthorName":"胡少坚"}],"doi":"10.3969/j.issn.1007-4252.2004.04.012","fpage":"455","id":"a767d909-c153-4f41-8e02-83c87bee360b","issue":"4","journal":{"abbrevTitle":"GNCLYQJXB","coverImgSrc":"journal/img/cover/GNCLYQJXB.jpg","id":"34","issnPpub":"1007-4252","publisherId":"GNCLYQJXB","title":"功能材料与器件学报 "},"keywords":[{"id":"1f2278b5-88b2-4b64-8ae6-9c0b6340ad47","keyword":"霍尔效应","originalKeyword":"霍尔效应"},{"id":"4a9ee7d5-a783-49d4-a18c-c7610fe6b431","keyword":"磁传感器","originalKeyword":"磁传感器"},{"id":"6c409367-91c7-4fa1-8e4e-9b9aba54281a","keyword":"不等位电势","originalKeyword":"不等位电势"}],"language":"zh","publisherId":"gnclyqjxb200404012","title":"GaAs霍尔元件不等位电势的调制消除","volume":"10","year":"2004"}],"totalpage":1250,"totalrecord":12500}