电荷密度

激发态对C（60）价电荷密度的影响

The Effect on the Valence Charge Density of C_ ( 60 ) Brought by s ~ Excited State

在掺杂剂附近的碳原子上出现较大的电荷密度，且p型比n型掺杂剂的影响更大。

There are large charge density on the carbon atoms near the dopant , and the effects of p-type dopants are greater than those of n-type ones .

讨论了K空位形成后电荷密度的重新分布、相应的电子态密度和能带结构等性质。

The properties of density of states and band structure on KDP with K vacancy were discussed .

电荷密度波材料K（0.3）MoO3及W掺杂样品的红外光学响应的研究

Infrared response of pure and W-doped K_ ( 0.3 ) MoO_3

用原子的Xα电荷密度计算vanderwaals半径

The Calculation of van der Waals Radii With the Atomic X_ α Densites

通过拟合计算出了绝缘埋层（BOX，即埋氧）中的饱和净正电荷密度Not和空穴俘获分数α。

The saturated net positive charge density N_ ( ot ) and the fraction of hole capture α in buried oxides are calculated by data fitting .

~（40）Ca的核子密度、动能密度、自旋密度和电荷密度的壳模型计算

Calculations of nucleon densities , kinetic energy densities , spin densities and charge density with shell model for ~ ( 40 ) ca

随着硅片表面电荷密度增加，BSA吸附量增加。

As the surface charge density increased , the adsorbed BSA amount also increased .

有源网络的拓扑分析PAC及其复合物电荷密度的影响因素分析

Topological Analysis of Active Network Application of High Charge Density PAC in Neutral Papermaking

高电荷密度的聚乙烯亚胺的加入能够中和DCS中的阴离子垃圾，提高阳离子聚丙烯酰胺的助留效果。

PEI with high cationic charge density could neutralize the anionic trash in DCS and improve the efficiency of CPAM .

另外，计入U、V使得电荷密度发生了重新分布，而且在缺陷及其周围格点上出现了束缚电荷；费米能级向能量升高的方向移动，并且在新的费米能级点出现了电子局域态。

Coulomb interaction V causes the inhomogeneous distribution of charge density , Fermi energy shift to high energy position and new Localized states appears .

准一维电荷密度波导体Rb（0.3）MoO3的低温电输运性质

Low-Temperature Electronic Transport Property of Quasi-One-Dimensional Charge-Density-Wave Conductor Rb_ ( 0.3 ) MoO_3

采用C-V法测量Si/GaP（Ⅲ）异质结的表观载流子浓度分布n（x），从中导出了异质界面的导带失配值和界面电荷密度。

The conduction band offset and the interface charge density are derived from the apparent carrier concentration distribution obtained by the C-V profiling techniqe .

水凝胶纳米粒子在32℃左右发生体积相转变，表面电荷密度同时具有温度和pH依赖性。

Their volume phase transition temperature was found to be around 32C , and the charge density on their surface is dependent on temperature and pH of the aqueous medium .

定量电子晶体学硼对Ni3Al的电荷密度分布的影响

Quantitative electron crystallography the effect of Boron on charge density distribution in ni_3al

通过X射线粉末衍射和透射电镜研究了在青霉素酰化酶（PGA）作用下双金属复合氧化物（LDO）记忆效应与其组成（层板电荷密度、层板离子种类）的关系。

Layered double oxide ( LDO ) immobilized penicillin G acylase ( PGA ) has been studied by XRD and TEM .

分析了得到的各原子分态密度、面电荷密度分布以及表面能带结构等性质，比较了GaN（001）的Ga端表面和N端表面两种情况。

Atomic partial densities of states , charge density distributions , and surface band structures are calculated and analyzed on both Ga terminated surface and N terminated surface .

MX络合物中电荷密度波和自旋密度波对三次谐波产生系数的影响

Effect of charge density wave and spin density wave on the third harmonic generation in MX complex

EuMo6S8的超导性、电荷密度波和磁性间的相互影响

Interplay among superconductivity , charge density waves , and magnetism in eumo_6s_8

吸附PAM后纳米SiO2的表面电荷密度、扩散层电荷密度以及ζ电位发生变化。

Surface charge density , diffuse charge density and measured zeta potential of SiO_ ( 2 ) particles vary distinctly after PAM adsorption .

随着载银二氧化钛的质量增加喷射流电荷密度增大，使PU静电纺丝纤维平均直径减小。

The addition of Ag-loaded titanium dioxide increased the charge density in the jets and resulted in the diameter of the PU electrospun fibers became smaller .

研究表明用密度泛函理论预测的不同膜面电荷密度和不同离子直径比情况下离子在半透膜附近密度分布与MonteCarlo模拟数据符合得很好。

The ionic density profiles predicted by the density functional theory are in excellent agreement with Monte Carlo results for various membrane surface charge densities and ionic diameter ratios .

一维金属中的Peierls相变和电荷密度波相变

The Peierls transition and the charge-density-wave transition in one-dimensional metals

表面等离子体波共振（SPR）是被入射电磁波所激发、存在于金属和电介质界面上电荷密度振动的谐振波。

Surface plasmon resonance ( SPR ) is used to describe the excitation and propagation of electromagnetic waves along the metal-dielectric interface .

结论：蒙脱石对CAG大鼠具有比硫糖铝更加明显的治疗作用，并且这种作用与蒙脱石的平均层电荷密度呈正相关。

Conclusion : The effectiveness of montmorillonite for the treatment of CAG seemed positive proportion to the average layer charge density of montmorillonite .

结果表明，当V增大到某一临界值时，铁磁基态变得不稳定，同时系统从自旋密度波态过渡到电荷密度波态。

The result shows that if the intersite Coulomb interaction V is larger than a critical value , the ground state is unstable and the transition from the spin-density-wave state to the charge-density-wave state occurs .

研究了BCTMP的物理化学特性及其对ASA中性施胶的影响。研究结果表明：BCTMP含有较多的细小组分，这些细小组分的比表面积较大且负电荷密度较高，对ASA的施胶不利；

In this paper , the physical-chemical characteristics of BCTMP and its effect on neutral sizing with ASA were studied .

然而，与PAM相比，壳聚糖的相对分子质量和电荷密度均较小，因此在絮凝时形成的絮体较小、结构较松散。

However , compared with PAM , molecular weight and charge density of chitosan are lower , so flocs formed in flocculation are smaller and less incompact .

电荷密度波电输运方程&Grüner方程解的周期性

Relation Between Transportation of Charge Density Wave and Periodic Solution of Gr ü ner ′ s Equation

通过Gouy-Chapman和Healy模化处理，揭示了α-Al2O3微粒固-液界面双电层电荷密度和厚度的分布状况。

The charge density distribution and the double-layer thickness were calculated by using Gouy-Chapman model .