{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"束缚态β-衰变是一种特殊的弱相互作用衰变模式,对某些高电离态重原子的β-衰变有重要或决定性的贡献. 从理论和实验两方面介绍了束缚态β-衰变研究的进展及其对恒星中的慢中子俘获过程和187Re-187Os宇宙核钟的影响.","authors":[{"authorName":"白希祥","id":"4f8a6773-0f6c-4cc9-8c6e-20abf7c3b46c","originalAuthorName":"白希祥"}],"doi":"10.3969/j.issn.1007-4627.2003.01.002","fpage":"11","id":"7f4aa80f-64a9-4328-958d-707b0b450ce1","issue":"1","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"f6d17ab8-8ac5-4dd7-8578-1fc239c5c7c4","keyword":"高电离态原子","originalKeyword":"高电离态原子"},{"id":"4377c4cc-f792-4605-b767-334b0d352b10","keyword":"束缚态 β-衰变","originalKeyword":"束缚态 β-衰变"},{"id":"e823abf9-b971-4150-9d2d-28f63debf1f1","keyword":"s中子俘获过程","originalKeyword":"s中子俘获过程"},{"id":"ac8dd7b1-b333-4a1a-8824-b073020bdeef","keyword":"宇宙核钟","originalKeyword":"宇宙核钟"}],"language":"zh","publisherId":"yzhwlpl200301002","title":"束缚态β-衰变及其天体物理意义","volume":"20","year":"2003"},{"abstractinfo":"主要报导用束箔技术对天体等离子体中重要元素硫的高电离态原子n=2的某些能级寿命的实验测量. 实验数据用CANDY程序分析, 并与理论计算结果和其它的实验结果作了比较. ","authors":[{"authorName":"杨治虎","id":"beb0bcd0-8ba6-402f-b0df-2995586c0192","originalAuthorName":"杨治虎"},{"authorName":"马新文","id":"2b56e857-8197-4f39-b399-9527d41b5ae5","originalAuthorName":"马新文"},{"authorName":"刘惠萍","id":"d9db5144-21d9-44f8-a28f-91abff95f8ef","originalAuthorName":"刘惠萍"},{"authorName":"王友德","id":"98c63acf-764b-4327-ab06-af3ea6457a7a","originalAuthorName":"王友德"},{"authorName":"苏弘","id":"fe6d32fc-f85a-42a1-a806-07c4f92179d7","originalAuthorName":"苏弘"},{"authorName":"肖国青","id":"bb342d63-bf55-409c-ae44-f5ca804c2428","originalAuthorName":"肖国青"}],"doi":"10.3969/j.issn.1007-4627.2002.02.011","fpage":"122","id":"b81a409c-9b40-48c6-bee2-6097e4fe2e31","issue":"2","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"76a1a56a-8a7e-499c-9c30-1837314c8a39","keyword":"束-箔技术","originalKeyword":"束-箔技术"},{"id":"8a545cd8-601a-444f-bc45-94f7ce6f021b","keyword":"高电离态原子","originalKeyword":"高电离态原子"},{"id":"1a4082b9-d513-4f65-93f0-85c19c32e651","keyword":"能级寿命","originalKeyword":"能级寿命"}],"language":"zh","publisherId":"yzhwlpl200202011","title":"类铍硫n=2的某些能级寿命的实验研究","volume":"19","year":"2002"},{"abstractinfo":"简要介绍了兰州重离子加速器上的高电离态原子光谱实验测量和取得的部分实验结果.","authors":[{"authorName":"杨治虎","id":"b3b6c733-70ee-4bea-9bcd-aff3801095c0","originalAuthorName":"杨治虎"},{"authorName":"苏弘","id":"499eb237-8ea4-4bb1-9f46-4058a4f05289","originalAuthorName":"苏弘"},{"authorName":"马新文","id":"9ca7e882-5c2a-41d2-8776-bd1d8e83831d","originalAuthorName":"马新文"},{"authorName":"刘惠萍","id":"0837732a-6b2f-42e0-b47e-1c2c177547fe","originalAuthorName":"刘惠萍"},{"authorName":"王友德","id":"e40354cc-c5a5-4c1c-b5ae-81693d87fc2b","originalAuthorName":"王友德"}],"doi":"10.3969/j.issn.1007-4627.2000.03.012","fpage":"183","id":"910d0e40-0598-4e76-988d-10f0f0c663d5","issue":"3","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"19cd6306-3c25-4605-b9f0-f43356993c06","keyword":"高电离态离子","originalKeyword":"高电离态离子"},{"id":"3464754b-0324-47d4-8e67-1788e8444d88","keyword":"激发光谱","originalKeyword":"激发光谱"},{"id":"2b1ef2a7-5812-4c4e-bbb4-566a89607ed6","keyword":"能级寿命","originalKeyword":"能级寿命"}],"language":"zh","publisherId":"yzhwlpl200003012","title":"高电离态原子光谱测量","volume":"17","year":"2000"},{"abstractinfo":"描述了用于高电离态原子光谱和能级寿命测量的计算机自动测量控制系统.介绍了系统的工作原理、总体设计, 给出了实验结果. ","authors":[{"authorName":"李宁溪","id":"a9f2bbc3-f61c-45b9-b605-2730311c2b61","originalAuthorName":"李宁溪"},{"authorName":"杨治虎","id":"f0fe0d97-2b68-48c6-83b2-d73b7aa95646","originalAuthorName":"杨治虎"},{"authorName":"黄新民","id":"155d5d1e-949a-477d-bfe0-441aa0f027ba","originalAuthorName":"黄新民"},{"authorName":"苏弘","id":"9cf55281-2434-485b-bc44-b9b62132318f","originalAuthorName":"苏弘"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.006","fpage":"17","id":"28052824-94d0-452d-b8ae-2fe113243ca5","issue":"z1","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"510c2788-1798-4650-987c-bfc6383df803","keyword":"光谱学","originalKeyword":"光谱学"},{"id":"c3710122-e8c4-4e32-b363-73a83acb7504","keyword":"重元素","originalKeyword":"重元素"},{"id":"8e15ef6f-3e08-4c0d-98f7-646cfce7ff76","keyword":"自动测量控制","originalKeyword":"自动测量控制"}],"language":"zh","publisherId":"yzhwlpl2002z1006","title":"高电离态原子光谱和能级寿命自动测量控制系统","volume":"19","year":"2002"},{"abstractinfo":"基于多组态Dirac-Fock方法的程序包GRASP92和RATIP及在此基础上最新发展的RELPHOTO08程序,系统地研究了高离化态金离子M壳层的光电离截面随入射光子能量、离化度以及壳层的变化规律.结果表明:光电离截面随光子能量的增大而单调减小;电离nl电子时,如果相关电子的主量子数较大,则该电子存在与否对其光电离截面几乎没有影响;在同一离化度下,角量子数l可引起两种性质不同的效应,其相互竞争可导致光电离截面随入射光子能量的复杂变化.","authors":[{"authorName":"王云荣","id":"e9fb7848-61f3-401a-be21-645c3d69331d","originalAuthorName":"王云荣"},{"authorName":"刘晓斌","id":"72af393e-f2ba-41e1-8823-f9aa7d6c3bef","originalAuthorName":"刘晓斌"},{"authorName":"丁晓彬","id":"5cf84fbc-7ee8-46b7-9d1d-17b3f3027a0e","originalAuthorName":"丁晓彬"},{"authorName":"董晨钟","id":"3635b01c-8016-4c04-bdbd-c0083c204afe","originalAuthorName":"董晨钟"}],"doi":"","fpage":"245","id":"27bae525-8d72-4324-ad34-5fd9c4aa5025","issue":"2","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"3e8bd991-1ea9-473e-9aaa-c93f82d1c257","keyword":"多组态Dirac-Fock方法","originalKeyword":"多组态Dirac-Fock方法"},{"id":"3aec22c9-2477-484d-a639-977ce7e67f61","keyword":"光电离","originalKeyword":"光电离"},{"id":"cb729554-3660-4a74-af4a-9191af7f7cf2","keyword":"截面","originalKeyword":"截面"}],"language":"zh","publisherId":"yzhwlpl201102020","title":"高离化态Au离子光电离过程的理论研究","volume":"28","year":"2011"},{"abstractinfo":"利用扭曲波Born交换近似方法, 系统地计算了Ar的类氢到类钠离子的电子碰撞电离截面和速率系数. 同时使用精度高的拟合公式对直接电离截面、激发截面、总激发自电离截面和速率系数进行了拟合, 以满足实际应用的需要. ","authors":[{"authorName":"赵永","id":"99e458c3-9de0-4a8d-8da7-6dedc6f7a9c9","originalAuthorName":"赵永"},{"authorName":"陈重阳","id":"892b3de4-c5d6-415e-9af7-e0b2c070816c","originalAuthorName":"陈重阳"},{"authorName":"王炎森","id":"c2a7584d-a5cb-44cf-88d9-692faeb7c7f9","originalAuthorName":"王炎森"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.018","fpage":"55","id":"9f32a511-3105-4d90-8ad9-33473c7f831e","issue":"z1","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"ca2971a6-74b2-4281-b40f-c29f8c95001d","keyword":"高电荷态离子","originalKeyword":"高电荷态离子"},{"id":"ea84a88e-8f2d-43af-a202-019fd9d2206c","keyword":"碰撞电离截面","originalKeyword":"碰撞电离截面"},{"id":"ac96fe1c-6b9e-4829-b646-02aa8eead2d4","keyword":"扭曲波近似","originalKeyword":"扭曲波近似"},{"id":"b3a7566d-2f86-4e85-ab32-6cc15c1e197e","keyword":"拟合公式","originalKeyword":"拟合公式"}],"language":"zh","publisherId":"yzhwlpl2002z1018","title":"电子与Ar的高电荷态离子的碰撞电离","volume":"19","year":"2002"},{"abstractinfo":"以Rayleigh-Ritz变分法以及组态相互作用为理论基础,选取Hylleraas基为基元,计算了氦原子高激发态能级结构,精度达到10-4以上.在低激发态时,计算结果与Drake的计算结果比较接近,在高L高激发态时,符合理论预期.此外,选取L=10激发态为样本,分析了氦原子在第十个激发态时能量收敛情况.通过分析,随着基组的扩大,能量收敛于一个固定数值,从而证明了计算结果的可靠性.最后,选取L=10激发态为样本,分析了氦原子处于高激发态时分波对应的关联度和能量贡献度.经过计算,(0,L)L组态贡献度最大,而其他分波的贡献则很小.因此,组态相互作用法可应用于氦原子的高激发态计算.","authors":[{"authorName":"牟健宇","id":"0a26142a-bcaf-4ecf-89ce-69188d6d0848","originalAuthorName":"牟健宇"},{"authorName":"乔豪学","id":"d52dead9-aa58-4bdb-a260-83225e391835","originalAuthorName":"乔豪学"}],"doi":"10.3969/j.issn.1007-5461.2013.06.005","fpage":"673","id":"7513aaff-1e6c-4f9d-a2f2-54915011ab6e","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":"071b6c0d-636e-4b61-94c4-a6063bcafe07","keyword":"光谱学","originalKeyword":"光谱学"},{"id":"bec4e702-9553-47c1-b6ce-218c5e402aa2","keyword":"氦原子","originalKeyword":"氦原子"},{"id":"4ef9dd31-0f7c-425b-a51a-9c936bc8edd2","keyword":"高激发态","originalKeyword":"高激发态"},{"id":"f61859fc-a07e-4e34-a572-b431e962152a","keyword":"变分法","originalKeyword":"变分法"}],"language":"zh","publisherId":"lzdzxb201306005","title":"氦原子高激发态的精确计算","volume":"30","year":"2013"},{"abstractinfo":"利用相对论性多通道量子亏损理论计算了Sc的原子里德堡态能级. 计算结果显示, 由于通道间的相互作用, 使得光谱非常复杂, 这与实验测量结果是一致的. ","authors":[{"authorName":"张新峰","id":"c1a6abf0-f456-4200-b566-f63ee07278f7","originalAuthorName":"张新峰"},{"authorName":"夏丹","id":"1f6ff1ed-a2b7-49f2-9803-e16b9c3e5dd4","originalAuthorName":"夏丹"},{"authorName":"钟志萍","id":"c5abb058-2edc-4b96-a837-189b375898e5","originalAuthorName":"钟志萍"},{"authorName":"彭永伦","id":"c94117f7-2a3e-4a23-80b7-7ed4e3de654d","originalAuthorName":"彭永伦"},{"authorName":"许祥源","id":"4e57b065-87b0-4e5b-b662-579297d3aa70","originalAuthorName":"许祥源"},{"authorName":"李家明","id":"12f03c7c-1ec8-4f84-a3a1-7c2ea1404ce7","originalAuthorName":"李家明"}],"doi":"10.3969/j.issn.1007-4627.2002.02.030","fpage":"192","id":"1d27f12c-358d-4088-a858-c9d2a703b247","issue":"2","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"67bfd691-38a6-47a0-92df-eda93f0627c0","keyword":"相对论性多通道量子亏损理论","originalKeyword":"相对论性多通道量子亏损理论"},{"id":"6650f753-63ea-49cf-8848-cd0a9ee8eaec","keyword":"Sc原子","originalKeyword":"Sc原子"},{"id":"97605cdd-33da-4327-9f01-d35ab4c0d0bf","keyword":"激发态","originalKeyword":"激发态"}],"language":"zh","publisherId":"yzhwlpl200202030","title":"Sc原子高激发态理论研究","volume":"19","year":"2002"},{"abstractinfo":"利用相对论平均自洽场理论,研究了相对论波函数的小分量对原子光电离截面的影响.原子核尺寸效应将使波函数小分量对原子光电离截面的影响减弱.由于波函数沿径向空间被压缩,电子离核的平均半径较小,波函数小分量对高离化态离子光电离截面的影响比对一般原子要强得多.波函数小分量反映了相对论效应的基本特征,从而也定性地说明了光电离过程中相对论效应的强弱.","authors":[{"authorName":"刘晓斌","id":"03fdd680-20e0-4a06-8367-d4947e6a79bf","originalAuthorName":"刘晓斌"},{"authorName":"邢永忠","id":"29102ba4-aca1-41d1-bf8a-ed072109dd73","originalAuthorName":"邢永忠"},{"authorName":"孙小伟","id":"9258b16f-80e3-43c7-a291-c29402ff068a","originalAuthorName":"孙小伟"}],"doi":"","fpage":"82","id":"e7244a6b-ff39-4029-b83e-3ea8d0445c00","issue":"1","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"ed49e503-e883-4fdd-a1a9-07161cbde118","keyword":"光电离","originalKeyword":"光电离"},{"id":"9481598f-0da1-4715-9c85-6568d9de2cc1","keyword":"截面","originalKeyword":"截面"},{"id":"a5b6866a-71b0-4171-976d-ba12054f00cd","keyword":"相对论效应","originalKeyword":"相对论效应"},{"id":"10a65310-1895-4991-a748-6b1929f8b670","keyword":"波函数小分量","originalKeyword":"波函数小分量"}],"language":"zh","publisherId":"yzhwlpl200801016","title":"相对论小分量波函数对原子光电离截面的影响","volume":"25","year":"2008"},{"abstractinfo":"在慢速高电荷态离子与氦原子碰撞的双电子转移过程中,借用虚态图像来描绘转移电子间的强关联特性;根据分子库仑过垒模型纳入反应Q值,定义势能参量ω来区分碰撞系统并度量双电子转移过程。对照之前的实验数据,清晰地显示当ω61和ω>2时,纯双电子俘获或自电离双俘获分别占优。澄清了碰撞系统的本质区别在于散射离子上两个转移电子的平均激发能和平均束缚能的相对比率。","authors":[{"authorName":"杜凡","id":"6464254c-8b85-42e4-9c25-70893e374efb","originalAuthorName":"杜凡"},{"authorName":"卢荣春","id":"35e43251-92ba-4052-ae45-eac39f22cd99","originalAuthorName":"卢荣春"},{"authorName":"于得洋","id":"8670b7d7-11aa-438a-9fee-1265e0c61da7","originalAuthorName":"于得洋"}],"doi":"10.11804/NuclPhysRev.31.02.224","fpage":"224","id":"34bab1c5-5b4a-4b32-ac62-822304de452a","issue":"2","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论 "},"keywords":[{"id":"ace2faea-1f34-4e7e-ba82-de1a799f74ed","keyword":"双电子转移","originalKeyword":"双电子转移"},{"id":"f1a2fb3e-2a55-4066-8118-46a10ba95f47","keyword":"纯双俘获","originalKeyword":"纯双俘获"},{"id":"f5c2dd70-c3a8-4b53-912e-1bd718bdbd7a","keyword":"自电离双俘获","originalKeyword":"自电离双俘获"},{"id":"15a376f8-8e06-4a0e-a8d4-97b0b8e84845","keyword":"双俘获稳定比","originalKeyword":"双俘获稳定比"}],"language":"zh","publisherId":"yzhwlpl201402018","title":"慢速高电荷态离子与氦原子碰撞中双俘获稳定比的势能参量","volume":"","year":"2014"}],"totalpage":3801,"totalrecord":38002}