{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"应用多源热模型研究了相对论性重离子对撞机(RHIC)上PHENIX合作组测得的每核子对质心能量(sNN)=200 GeV的氘-金(d+Au)碰撞中快度<span style=\"color:red\">长程</span><span style=\"color:red\">方位角</span><span style=\"color:red\">关联</span>,和大型强子对撞机(LHC)上CMS合作组测得的质心能量(s)=0.9,2.36,7 TeV的质子质子(p+p)碰撞中高多重数短程赝快度<span style=\"color:red\">关联</span>,在误差范围内模型结果很好地重现了实验数据.用4个参数分析了<span style=\"color:red\">长程</span><span style=\"color:red\">方位角</span><span style=\"color:red\">关联</span>,结果表明,参数可以清楚地显示出脊结构的变化趋势,说明脊结构与集体效应、流体力学流效应、粒子对的横动量及信号等有关.用3个参数分析了小系统高多重数短程赝快度<span style=\"color:red\">关联</span>,结果表明,参数σ和c3与能量相关,能量越大,两粒子越靠近,<span style=\"color:red\">关联</span>越强.","authors":[{"authorName":"司瑞芳","id":"7097fc53-0382-4690-ae7d-d128237080b2","originalAuthorName":"司瑞芳"},{"authorName":"刘福虎","id":"2705a90b-b4ad-4483-957f-34862a00425c","originalAuthorName":"刘福虎"}],"doi":"10.11804/NuclPhysRev.33.04.414","fpage":"414","id":"a84a109c-a5c5-4997-b312-5e3f8703a1f4","issue":"4","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":"d5137ea2-a39b-4c29-a644-536ec8e47abc","keyword":"多源热模型","originalKeyword":"多源热模型"},{"id":"3dd44b71-8012-4574-86d7-80e772d5a8d4","keyword":"<span style=\"color:red\">长程</span><span style=\"color:red\">方位角</span><span style=\"color:red\">关联</span>","originalKeyword":"长程方位角关联"},{"id":"7047185e-e02d-42db-9177-35f729586171","keyword":"短程赝快度<span style=\"color:red\">关联</span>","originalKeyword":"短程赝快度关联"}],"language":"zh","publisherId":"yzhwlpl201604005","title":"RHIC和LHC能区两粒子<span style=\"color:red\">关联</span>函数研究","volume":"33","year":"2016"},{"abstractinfo":"通过原位聚合法合成聚丙烯腈(PAN)/碳纳米管(CNT)复合溶液,经过湿法纺丝技术制备了PAN/CNT复合原丝.通过X射线衍射仪,扫描电子显微镜和单丝拉伸仪研究了CNTs对PAN纤维晶态结构及力学性能的影响.结果表明,在<span style=\"color:red\">方位角</span>扫描图中,随着PAN/CNT复合纤维的制备过程,其双峰的不对称性逐渐增加,其强度比从1.054增加到1.258;复合原丝的结晶度(53.10%)高于PAN原丝的结晶度(51.89%);在赤道扫描图中,PAN/CNT复合原丝的斜方晶系200晶面峰比PAN原丝明显,且晶粒尺寸高于PAN原丝;复合原丝的断面形貌出现更多的微纤结构,且比PAN原丝具有更高的拉伸模量.","authors":[{"authorName":"张海龙","id":"fac1f02f-ba2e-4079-a455-1ba85fdf6069","originalAuthorName":"张海龙"},{"authorName":"杨逢源","id":"a0ff3caf-8cf1-44ad-8dae-2d69449c0ef6","originalAuthorName":"杨逢源"},{"authorName":"李常清","id":"eeb67cc3-a899-4fb0-8aa9-bad1a621aa15","originalAuthorName":"李常清"},{"authorName":"徐樑华","id":"b6697baf-73df-4492-a1f8-42f5837d423c","originalAuthorName":"徐樑华"}],"doi":"","fpage":"671","id":"3126a559-3cbf-46d4-b9e8-4c5bb3fea9b9","issue":"4","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"213b8232-953c-448b-9bb1-0b6f93dd73b5","keyword":"聚丙烯腈","originalKeyword":"聚丙烯腈"},{"id":"643ec2d0-bc2c-4c12-bd53-7bc2a7139e89","keyword":"<span style=\"color:red\">方位角</span>","originalKeyword":"方位角"},{"id":"d7b2d2b8-d536-47e4-999e-f524ffa06a1e","keyword":"不对称","originalKeyword":"不对称"},{"id":"6e89c12d-ea02-445d-8513-c5a63ce2b30c","keyword":"碳纳米管","originalKeyword":"碳纳米管"},{"id":"00e17e1a-ed0e-4fa4-877b-3ec562de86e8","keyword":"复合纤维","originalKeyword":"复合纤维"}],"language":"zh","publisherId":"gncl201004033","title":"<span style=\"color:red\">方位角</span>不对称的PAN/CNT复合纤维的晶态结构与性能","volume":"41","year":"2010"},{"abstractinfo":"利用多源热模型分析了ATLAS实验组2.76 TeV铅-铅碰撞中产生的、带电粒子在多个不同中心度事例中的<span style=\"color:red\">方位角</span>分布，并与n=2,4,6和n=2的傅里叶级数形式的<span style=\"color:red\">方位角</span>分布进行了比较。同时，利用由多源热模型得到的散射源在横动量空间的结构参数，计算了散射源在横动量空间的各向异性率和相对膨胀率，且与相关傅里叶系数进行了比较。在各个中心度区间，横动量空间的各向异性率和相对膨胀率都小于相应的傅里叶系数，椭圆各向异性是末态<span style=\"color:red\">方位角</span>分布中最主要的成分，其他成分的各向异性在各中心度区间的贡献不同且作用不可忽视。","authors":[{"authorName":"司瑞芳","id":"009cf0ab-6120-4dee-8720-996598095351","originalAuthorName":"司瑞芳"},{"authorName":"刘福虎","id":"682eb51a-0999-4de6-934e-f497fbc77c02","originalAuthorName":"刘福虎"}],"doi":"10.11804/NuclPhysRev.32.04.392","fpage":"392","id":"4c4fc21e-a010-4e8e-9f11-374ad295e984","issue":"4","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":"0862cc6b-5f61-45de-9f6c-e83400ab68a2","keyword":"铅-铅碰撞","originalKeyword":"铅-铅碰撞"},{"id":"2a310ccc-1fbe-4299-8363-89c91b3cbfbb","keyword":"带电粒子","originalKeyword":"带电粒子"},{"id":"f9329047-ee5e-4ff6-a914-a33bc0e798b5","keyword":"<span style=\"color:red\">方位角</span>分布","originalKeyword":"方位角分布"},{"id":"2f9e1954-f36e-481f-9cd2-2acdab8d1af3","keyword":"多源热模型","originalKeyword":"多源热模型"}],"language":"zh","publisherId":"yzhwlpl201504004","title":"2.76 TeV铅-铅碰撞中带电粒子的<span style=\"color:red\">方位角</span>分布","volume":"32","year":"2015"},{"abstractinfo":"在较大的连续<span style=\"color:red\">角</span>区范围内测量了27Al+27Al耗散反应产物的激发函数,入射束流的能量从114 MeV到127 MeV,能量步长200 keV. 分析激发函数的角度<span style=\"color:red\">关联</span>,角度相干宽度超过40°,各个角度之间反应产物的互<span style=\"color:red\">关联</span>系数在0.6以上. 用宏观条件下的量子态叠加讨论了这种<span style=\"color:red\">长程</span>角度<span style=\"color:red\">关联</span>.","authors":[{"authorName":"王琦","id":"cdc17cd6-c395-4df1-a607-0ee0f64a39c1","originalAuthorName":"王琦"},{"authorName":"董玉川","id":"63a4b9e7-25f1-4e98-9b5e-c78fa00ee943","originalAuthorName":"董玉川"},{"authorName":"李松林","id":"e8ae0cfa-0939-4886-8837-70708a6e3ad7","originalAuthorName":"李松林"},{"authorName":"田文栋","id":"aee50adf-8112-473e-8073-7dadb011d4a6","originalAuthorName":"田文栋"},{"authorName":"高辉","id":"b60108e0-0f61-4466-9262-8df2c2bfe9c1","originalAuthorName":"高辉"}],"doi":"10.3969/j.issn.1007-4627.2003.01.004","fpage":"26","id":"737a5301-e261-4db7-b8ae-034861b9c77e","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":"571a0761-20d5-474a-a369-690a987c6f72","keyword":"耗散产物","originalKeyword":"耗散产物"},{"id":"51e300df-b658-4284-b039-7bff908c0c0a","keyword":"激发函数","originalKeyword":"激发函数"},{"id":"92435300-41d4-4ad4-ade8-681a22223ee9","keyword":"<span style=\"color:red\">长程</span>角度<span style=\"color:red\">关联</span>","originalKeyword":"长程角度关联"},{"id":"8a3568b7-a5a6-4be4-baf3-fc778e9d20b4","keyword":"量子态叠加","originalKeyword":"量子态叠加"}],"language":"zh","publisherId":"yzhwlpl200301004","title":"激发函数中的<span style=\"color:red\">长程</span>角度<span style=\"color:red\">关联</span>与量子态叠加","volume":"20","year":"2003"},{"abstractinfo":"本文实验研究了常压下液氮在多<span style=\"color:red\">方位</span>矩形窄缝通道中的沸腾传热特性.研究发现液氮在不同窄缝<span style=\"color:red\">方位角</span>时,壁面过热度有差异;窄缝间隙愈小,沸腾传热系数愈高.在中等热流密度下,强化传热作用明显,传热系数可达常规光管的3～5倍.加热面呈0°和180°放置时,在相同热流下其他角度尚处于核态沸腾区时,已达CHF点.","authors":[{"authorName":"尤国春","id":"1f7e0c34-ed18-40a8-a677-4ec5dbc1fd3b","originalAuthorName":"尤国春"},{"authorName":"张鹏","id":"87c7bbd5-2798-470a-b9f2-03f447c88cb8","originalAuthorName":"张鹏"},{"authorName":"王如竹","id":"a0f88a60-e951-4e7a-97f3-fe05a2d489dd","originalAuthorName":"王如竹"}],"doi":"","fpage":"472","id":"0aa0a793-8345-40a3-b5d6-668b299fde24","issue":"3","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":"b2fb41d3-af92-488c-b3c0-52363248b2b0","keyword":"多<span style=\"color:red\">方位</span>","originalKeyword":"多方位"},{"id":"21dd7fc8-20a0-4963-9e5a-d0b7d37efab9","keyword":"液氮","originalKeyword":"液氮"},{"id":"9371a99b-78e1-4a71-b20f-d8b6120957d6","keyword":"窄缝","originalKeyword":"窄缝"}],"language":"zh","publisherId":"gcrwlxb200403034","title":"多<span style=\"color:red\">方位</span>矩形窄缝中液氮沸腾传热特性实验研究","volume":"25","year":"2004"},{"abstractinfo":"介绍并分析了中高能核反应过程中与反应平面相关的可观测量, 以及确定核反应平面的各种方法. 这些方法包括裂变碎片<span style=\"color:red\">方位角</span>测量、类弹碎片测量、动量流球形张量、横向动量的方向性、<span style=\"color:red\">方位角</span><span style=\"color:red\">关联</span>和Fourier谐波分析等. ","authors":[{"authorName":"魏志勇","id":"60dfcf1d-004e-404a-be83-c1bce8b27c35","originalAuthorName":"魏志勇"},{"authorName":"靳根明","id":"8bb1e299-4c4c-499a-b17a-c0b75bd8cc16","originalAuthorName":"靳根明"},{"authorName":"诸永泰","id":"b7429bd3-c003-453d-967d-37f818426bba","originalAuthorName":"诸永泰"},{"authorName":"吴和宇","id":"cd053541-b2d7-4f76-888b-c015c693d44f","originalAuthorName":"吴和宇"}],"doi":"10.3969/j.issn.1007-4627.2002.01.007","fpage":"35","id":"05223e67-4f53-4221-8f05-da8fc5caccf5","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":"154d699a-9eb2-41c6-871b-daa658f5ca40","keyword":"反应平面","originalKeyword":"反应平面"},{"id":"47353bc7-e85c-43bc-8256-5bb0bd47d00b","keyword":"统计发射","originalKeyword":"统计发射"},{"id":"95e97ff5-80c6-4e1e-99c8-40dc87b1a7f7","keyword":"动力学发射","originalKeyword":"动力学发射"}],"language":"zh","publisherId":"yzhwlpl200201007","title":"中能核反应中反应平面的确定","volume":"19","year":"2002"},{"abstractinfo":"为了分析液晶光谱偏振系统的<span style=\"color:red\">方位</span>误差并降低测量误差,提出了选偏器<span style=\"color:red\">方位</span>误差的分析方法。该方法基于 Stokes矢量及 Mueller 矩阵,将偏振<span style=\"color:red\">角</span>的<span style=\"color:red\">方位</span>误差转化为 Stokes 矢量传递误差,推导了误差的协方差矩阵,分析了权重系数与延迟相位的变化关系,并对不同偏振态入射光条件下的品质因数变化进行了计算仿真。<span style=\"color:red\">方位</span>误差依赖于入射光 Stokes参数与延迟相位,不同偏振态的入射光品质因数随延迟相位成抛物线变化。当延迟相位位于[60°,120°]区间内,选偏器的<span style=\"color:red\">方位</span>误差较小,测量误差较小适宜测量。通过对液晶偏振光谱系统配准误差的研究,获得误差来源,为进一步提高系统测量精度奠定了理论基础。","authors":[{"authorName":"甘世奇","id":"da0ae095-ee86-4586-9688-6f5e47900ba1","originalAuthorName":"甘世奇"},{"authorName":"陈向宁","id":"90480d86-2c78-4f8e-a76f-5b4e018140b2","originalAuthorName":"陈向宁"},{"authorName":"薛俊诗","id":"8449801a-68b3-4085-8a5c-1c7e39656b62","originalAuthorName":"薛俊诗"},{"authorName":"赵融生","id":"24baf5b2-7d1d-4a39-b712-0562b826dfd1","originalAuthorName":"赵融生"}],"doi":"10.3788/YJYXS20163108.0748","fpage":"748","id":"b1b8ea3e-273c-472c-af6f-23f583d7de93","issue":"8","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示   "},"keywords":[{"id":"244cd9b3-f1ed-45d5-8771-9fd4ae723d97","keyword":"<span style=\"color:red\">方位</span>误差","originalKeyword":"方位误差"},{"id":"e1093fae-2162-4312-b29b-89ed595bcb03","keyword":"液晶偏振光谱系统","originalKeyword":"液晶偏振光谱系统"},{"id":"4eb83f9c-d654-490a-849c-4c6534d85650","keyword":"协方差矩阵","originalKeyword":"协方差矩阵"},{"id":"0e14f337-119b-4f6e-953d-d2aa9e44eddd","keyword":"Stokes 矢量","originalKeyword":"Stokes 矢量"}],"language":"zh","publisherId":"yjyxs201608003","title":"液晶光谱偏振系统选偏器<span style=\"color:red\">方位</span>误差研究","volume":"31","year":"2016"},{"abstractinfo":"按照一般的无序理论,在非<span style=\"color:red\">关联</span>一维无序材料中不存在扩展态,在绝对零度下,电子的波函数是局域的,系统表现为绝缘体.在<span style=\"color:red\">关联</span>无序系统中,格点能量之间的<span style=\"color:red\">长程</span><span style=\"color:red\">关联</span>,即对角<span style=\"color:red\">关联</span>,能导致扩展的波函数并由此导致系统的导电性.当<span style=\"color:red\">关联</span>强度于某一阈值,可以发现在热力学极限之下有存在于较宽能带范围内的扩展态,此阈值即为体系的金属-绝缘体转变临界点.考虑格点之间的<span style=\"color:red\">长程</span>相互作用势,即非对角<span style=\"color:red\">关联</span>时,在一维系统中通过使用传输矩阵方法,可以获得电子态的一些本质效应,<span style=\"color:red\">长程</span>跳跃可以改变系统的有效维度并能导出一维体系中存在有依赖于<span style=\"color:red\">关联</span>强度的金属-绝缘体转变.","authors":[{"authorName":"刘小良","id":"fffdbd43-b807-4484-9a17-35265efd47d6","originalAuthorName":"刘小良"},{"authorName":"徐慧","id":"a5d58645-bdf4-4200-95e9-b162922f0aa1","originalAuthorName":"徐慧"},{"authorName":"马松山","id":"cd9bfff4-4037-4aa2-b47b-d8120c19afb0","originalAuthorName":"马松山"},{"authorName":"肖剑荣","id":"f6329acd-73b1-4894-b3b7-f0bf800626e4","originalAuthorName":"肖剑荣"}],"doi":"","fpage":"20","id":"eb77b88f-0cba-45cc-a04c-06d45bbeccf5","issue":"9","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"be72d26b-4318-4c66-ae3d-1ee45917911f","keyword":"无序","originalKeyword":"无序"},{"id":"168ac7aa-e783-4cfa-9e26-0eae71217b5f","keyword":"<span style=\"color:red\">关联</span>","originalKeyword":"关联"},{"id":"2456331a-7c36-4add-aeac-405219a100fb","keyword":"<span style=\"color:red\">长程</span>跳跃","originalKeyword":"长程跳跃"},{"id":"40b298c3-ff4c-4ea1-98cb-5299214b330a","keyword":"金属-绝缘体转变","originalKeyword":"金属-绝缘体转变"}],"language":"zh","publisherId":"cldb200509006","title":"<span style=\"color:red\">关联</span>无序材料中电子态的研究方法","volume":"19","year":"2005"},{"abstractinfo":"本论文研究的全<span style=\"color:red\">方位</span>生长装置能解决常规的ADP晶体的单向生长问题.在这套装置中,籽晶完全位于溶液中央,籽晶可以首先恢复其理想的结晶学外形.在晶体生长过程中,晶体在各个方向的生长均为自由生长,且育晶器中央的溶液稳定性也明显高于育晶器顶部和底部.这些因素都有利于ADP晶体的优质快速生长.实验所得晶体的质量通过透过率、晶体内缺陷位错密度、高分辨率X射线衍射表征,并将所得结果与常规方法进行了比较.","authors":[{"authorName":"马江涛","id":"79ed0417-496c-43c0-8b7f-5251e9c9cdf2","originalAuthorName":"马江涛"},{"authorName":"滕冰","id":"1e9207d6-b2a8-4932-bf01-73f8ddc0f1af","originalAuthorName":"滕冰"},{"authorName":"钟德高","id":"5828cc27-8c9e-4ec1-983c-7805a3ac426a","originalAuthorName":"钟德高"},{"authorName":"曹丽凤","id":"08e6e816-b04a-4fd1-a4ce-840514bce81a","originalAuthorName":"曹丽凤"},{"authorName":"温吉龙","id":"c2c0cf4b-4675-4a97-8a40-4ea2a967adfc","originalAuthorName":"温吉龙"}],"doi":"","fpage":"1319","id":"eaa2d240-e1a8-4f06-8d0e-c9fb4f76447f","issue":"7","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":"b5e97b75-56da-413b-b18f-a71411370de5","keyword":"ADP晶体","originalKeyword":"ADP晶体"},{"id":"79221c1a-84d5-42f7-aca1-771362aadd68","keyword":"全<span style=\"color:red\">方位</span>生长","originalKeyword":"全方位生长"},{"id":"5ced2aeb-fee1-47a4-bea1-ca32b4141036","keyword":"理想外形","originalKeyword":"理想外形"},{"id":"ab4e22f6-5416-4655-98c3-8624e11fff47","keyword":"生长装置","originalKeyword":"生长装置"}],"language":"zh","publisherId":"rgjtxb98201307015","title":"ADP晶体的全<span style=\"color:red\">方位</span>生长装置","volume":"42","year":"2013"},{"abstractinfo":"采用一种全新的ADP晶体生长方法,使晶体首先恢复其理想外形,实现晶体的全<span style=\"color:red\">方位</span>生长,从而提高晶体的生长速度.并对所得晶体进行了透过率,激光散射,摇摆曲线测试及热重差热分析,与常规生长方法比较并分析了全<span style=\"color:red\">方位</span>生长方法的优势.","authors":[{"authorName":"马江涛","id":"7b3e06a1-98af-4f48-a3a7-f5875818d528","originalAuthorName":"马江涛"},{"authorName":"滕冰","id":"f976b6e7-a442-488b-8900-e36ec89d953c","originalAuthorName":"滕冰"},{"authorName":"钟德高","id":"48ecf2e4-0349-47e6-b1f3-95388f18fb30","originalAuthorName":"钟德高"},{"authorName":"曹丽凤","id":"992904d4-2406-47fd-9e3b-c10268acc634","originalAuthorName":"曹丽凤"},{"authorName":"温吉龙","id":"54fa7acf-3bb6-44eb-b1d9-412998fb373a","originalAuthorName":"温吉龙"},{"authorName":"","id":"9f232cd9-c7e0-4331-9f98-10b269afa759","originalAuthorName":""}],"doi":"","fpage":"208","id":"2624de4e-10cf-4499-a62b-a09676bf138c","issue":"2","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":"c3465726-54c3-470a-b44e-274d877d4860","keyword":"ADP晶体","originalKeyword":"ADP晶体"},{"id":"21ac5012-41a3-4511-bc7e-476e791867e3","keyword":"全<span style=\"color:red\">方位</span>生长","originalKeyword":"全方位生长"},{"id":"16387b2f-52e8-4e9c-b61f-571db81d91df","keyword":"理想外形","originalKeyword":"理想外形"},{"id":"37075751-d6c3-4e3d-8466-3efa38d474f7","keyword":"生长速度","originalKeyword":"生长速度"}],"language":"zh","publisherId":"rgjtxb98201302004","title":"ADP晶体的全<span style=\"color:red\">方位</span>生长方法研究","volume":"42","year":"2013"}],"totalpage":488,"totalrecord":4872}