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高抗渗水泥石的研究
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作者 岳云德 赵平 《中国建材科技》 1991年第3期51-58,共8页
通过X射线愆射、差热、扫描电镜、测孔仪分析等研究了高抗渗水泥水化产物,微观密实结构,水泥石总孔隙率与抗渗透性能的发展关系。结果表明,水化产物主要是C-S-H、钙矾石、Ca(OH)_2。水泥水化硬化过程中生成的钙矾石,能填充、堵塞水泥石... 通过X射线愆射、差热、扫描电镜、测孔仪分析等研究了高抗渗水泥水化产物,微观密实结构,水泥石总孔隙率与抗渗透性能的发展关系。结果表明,水化产物主要是C-S-H、钙矾石、Ca(OH)_2。水泥水化硬化过程中生成的钙矾石,能填充、堵塞水泥石中的毛细孔缝。而钙矾石的形貌特征对水泥石的抗渗透有着影响,密聚型钙矾石对抗渗透的作用更加显著。 展开更多
关键词 高抗渗 微观 抗渗透 密聚型
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A New Calculation of the In-Medium Quark Condensate at Finite Density and Temperature 被引量:2
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作者 唐欢欢 彭光雄 《Communications in Theoretical Physics》 SCIE CAS CSCD 2011年第12期1071-1074,共4页
The in-medium quark condensate is studied with an equivalent-mass approach in which one does not need to make assumptions on the derivatives of model parameters with respect to the quark current mass.It is shown that ... The in-medium quark condensate is studied with an equivalent-mass approach in which one does not need to make assumptions on the derivatives of model parameters with respect to the quark current mass.It is shown that the condensate is generally a decreasing function of both the density and temperature with the decreasing speed depending on the confinement parameter.Specially,at given density,the condensate decreases on increasing temperature.The decreasing speed is comparatively small at lower temperature,and becomes very fast at higher temperature. 展开更多
关键词 in-medium quark condensate equivalent-mass chiral symmetry breaking
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A New Selective Neural Network Ensemble Method Based on Error Vectorization and Its Application in High-density Polyethylene (HDPE) Cascade Reaction Process
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作者 朱群雄 赵乃伟 徐圆 《Chinese Journal of Chemical Engineering》 SCIE EI CAS CSCD 2012年第6期1142-1147,共6页
Chemical processes are complex, for which traditional neural network models usually can not lead to satisfactory accuracy. Selective neural network ensemble is an effective way to enhance the generalization accuracy o... Chemical processes are complex, for which traditional neural network models usually can not lead to satisfactory accuracy. Selective neural network ensemble is an effective way to enhance the generalization accuracy of networks, but there are some problems, e.g., lacking of unified definition of diversity among component neural networks and difficult to improve the accuracy by selecting if the diversities of available networks are small. In this study, the output errors of networks are vectorized, the diversity of networks is defined based on the error vectors, and the size of ensemble is analyzed. Then an error vectorization based selective neural network ensemble (EVSNE) is proposed, in which the error vector of each network can offset that of the other networks by training the component networks orderly. Thus the component networks have large diversity. Experiments and comparisons over standard data sets and actual chemical process data set for production of high-density polyethylene demonstrate that EVSNE performs better in generalization ability. 展开更多
关键词 high-density polyethylene modeling selective neural network ensemble diversity definition error vectorization
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Reanalysis of the Z_c(4020), Z_c(4025), Z(4050) and Z(4250) as Tetraquark States with QCD Sum Rules
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作者 王志刚 《Communications in Theoretical Physics》 SCIE CAS CSCD 2015年第4期466-480,共15页
In this article, we calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the C γμ- Cγνtype scalar, axial-vector and tensor tetraquark states in deta... In this article, we calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the C γμ- Cγνtype scalar, axial-vector and tensor tetraquark states in details with the QCD sum rules. In calculations, we use the formula μ = √M^2X/ Y /Z-(2Mc)^2 to determine the energy scales of the QCD spectral densities. The predictions MJ =2=(4.02-0.09^+0.09) GeV, MJ =1=(4.02-0.08^+0.07) GeV favor assigning the Zc(4020) and Zc(4025) as the J^PC= 1^+-or 2^++diquark-antidiquark type tetraquark states, while the prediction MJ =0=(3.85-0.09^+0.15) GeV disfavors assigning the Z(4050) and Z(4250) as the J^P C= 0^++ diquark-antidiquark type tetraquark states. Furthermore, we discuss the strong decays of the 0^++, 1^+-, 2^++diquark-antidiquark type tetraquark states in details. 展开更多
关键词 tetraquark state QCD sum rules
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