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国家自然科学基金(11074176)

作品数:10 被引量:16H指数:3
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10 条 记 录,以下是 1-10
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氮化铝分子及氯化锂分子结合能的量子蒙特卡罗研究
2012年
通过量子蒙特卡罗方法(QMC)利用不同的密度泛函轨道对氮化铝分子及氯化锂分子的结合能进行研究.采用扩散蒙特卡罗方法(DMC)得到氮化铝分子的结合能为2.993 eV,氯化锂分子的结合能为6.694 eV.与其他理论计算相比较,更接近实验得到氮化铝和氯化锂分子的结合能(2.862±0.391 eV和6.646 eV).同时,利用密度泛函理论对氮化铝分子及氯化锂分子的结合能进行研究时发现,利用密度泛函理论计算得到的结合能范围跨度很大且非常不准确.另外,在利用量子蒙特卡罗方法的计算中发现,不同类型的密度泛函轨道对结合能的计算产生一定的影响,这就需要在利用量子蒙特卡罗方法进行计算时考虑轨道的选择.
徐书伟程新路冯世全陈晓旭
关键词:结合能
反应分子动力学模拟研究冲击速度对RDX分解过程的影响(英文)
利用ReaxFF反应分子动力学模拟方法研究了冲击速度对RDX分解过程的影响。讨论了完整的RDX分子和关键产物随时间的变化演示过程,同时给出了系统温度在不同冲击速度作用下的变化情况。通过研究模拟胞尺寸大小对RDX分解产物的...
陈芳张红曹端林程新路
关键词:RDXREAXFF热分解
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石墨烯量子点二聚物的等离激元激发被引量:1
2014年
基于含时密度泛函理论,研究了石墨烯量子点二聚物的等离激元激发.当2个石墨烯量子点靠近,若量子点间的间隙较大,通过电容性相互作用时,石墨烯量子点二聚物的低能等离激元共振模式随着间隙的减小发生红移.进一步减小间隙时,由于电子的隧穿,二聚物的等离激元共振模式发生了改变,杂化等离激元共振模式形成.杂化等离激元共振模式随着间隙的减小继续红移.石墨烯量子点二聚物等离激元共振模式的演化规律不依赖于石墨烯量子点的形状.
尹海峰张红刘丹丹
关键词:等离激元含时密度泛函理论
X-ray spectra of high temperature tungsten plasma calculated with collisional radiative model
2013年
Tungsten is regarded as an important candidate of plasma facing material in international thermonuclear experimental reactor (ITER), so the determination and modeling of spectra of tungsten plasma, especially the spectra at high temperature were intensely focused on recently. In this work, using the atomic structure code of Cowan, a collisional radiative model (CRM) based on the spin-orbit-split-arrays is developed. Based on this model, the charge state distribution of tungsten ions is determined and the soft X-ray spectra from high charged ions of tungsten at different temperatures are calculated. The results show that both the average ionization charge and line positions are well agreed with others calculations and measurements with discrepancies of less than 0.63% and 1.26%, respectively. The spectra at higher temperatures are also reported and the relationship between ion abundance and temperature is predicted in this work.
王君张红程新路
关键词:面向等离子体材料X射线光谱国际热核实验反应堆高电荷态离子
Ar adsorptions on Al (111) and Ir (111) surfaces:a first-principles study
2012年
We investigate the adsorptions of Ar on Al (111) and Ir (111) surfaces at the four high symmetry sites,i.e.,top,bridge,fcc-and hcp-hollow sites at the coverage of 0.25 monolayer (ML) using the density functional theory within the generalized gradient approximation of Perdew,Burke and Ernzerhof functions.The geometric structures,the binding energies,the electronic properties of argon atoms adsorbed on Al (111) and Ir (111) surfaces,the difference in electron density between on the Al (111) surface and on the Ir (111) surface and the total density of states are calculated.Our studies indicate that the most stable adsorption site of Ar on the Al (111) surface is found to be the fcc-hollow site for the (2 × 2) structure.The corresponding binding energy of an argon atom at this site is 0.538 eV/Ar atom at a coverage of 0.25 ML.For the Ar adsorption on Ir (111) surface at the same coverage,the most favourable site is the hcp-hollow site,with a corresponding binding energy of 0.493 eV.The total density of states (TDOS) is analysed for Ar adsorption on Al (111) surface and it is concluded that the adsorption behaviour is dominated by the interaction between 3s,3p orbits of Ar atom and the 3p orbit of the base Al metal and the formation of sp hybrid orbital.For Ar adsorption on Ir (111) surface,the conclusion is that the main interaction in the process of Ar adsorption on Ir (111) surface comes from the 3s and 3p orbits of argon atom and 5d orbit of Ir atom.
牛纹霞张红
关键词:氩原子ALIR杂化轨道广义梯度近似
氮掺杂六角石墨烯纳米结构的近红外等离激元研究被引量:3
2014年
基于含时密度泛函理论研究了氮掺杂六角石墨烯纳米结构的近红外等离激元.沿一定的激发方向,边长为1 nm的氮掺杂六角石墨烯纳米结构在整个近红外光谱区都有强度较大的等离激元共振.参与这种近红外等离激元模式共振的电子在六角纳米结构的中心和边缘区域之间来回振荡.近红外等离激元共振模式的形成依赖于氮掺杂的位置和纳米结构的尺度大小.只有当氮掺杂在靠近边界区域时体系才会在近红外光谱区形成等离激元共振模式.对于边长小于1 nm的六角石墨烯纳米结构,氮掺杂后体系不能在近红外光谱区形成等离激元共振模式.
尹海峰张红岳莉
关键词:等离激元近红外光谱含时密度泛函理论
Hydrogen Adsorption on Ti Decorating Benzene Grafted Tetrahydrido-silsequioxanes
2012年
A novel type of Ti decorating benzene grafted tetrahydrido-silsequioxane struc-tures was designed and investigated using density functional theory(DFT).The hydrogen adsorption properties of this new material were investigated at the same level of theory.The results reveal that up to four hydrogen molecules(with the restrict of 18 electrons rule) can be adsorbed on each Ti atom of(TiC6H5)m-H4-mSi4O6(m = 1-4) molecular systems with the average binding energies of 0.691,0.692,0.693 and 0.695 eV for m = 1-4,respectively.The variations of HOMO- LUMO energy gaps verify that the host structures with four H2 molecules adsorbed own the best kinetics stability.The interaction mechanism of H2 molecules with the host materials mainly attributes to the well-known "kubas interactions".All the results indicate that the complex structures designed here may be used as hydrogen storage materials at ambient conditions.
李晓东张红唐永建吴卫东王朝阳
关键词:氢吸附钛原子嫁接密度泛函理论动力学稳定性
First-principles study of Ar adsorptions on the (111) surfaces of Pd, Pt, Cu, and Rh
2013年
In the present paper we give a detailed report on the results of our first-principles investigations of Ar adsorptions at the four high symmetry sites on M(111)(M = Pd,Pt,Cu,and Rh) surfaces.Our studies indicate that the most stable adsorption sites of Ar on Pd(111) and Pt(111) surfaces are found to be the fcc-hollow sites.However,for Ar adsorptions on Cu(111) and Rh(111) surfaces,the most favorable site is the on-top site.The density of states(DOS) is analyzed for Ar adsorption on M(111) surfaces,and it is concluded that the adsorption behavior is dominated by the interaction between 3s,3p orbits of Ar atoms and the d orbit of the base metal atoms.
牛纹霞张红龚敏程新路
关键词:THEORYBINDINGELECTRONIC
C_(60)富勒烯二聚物的等离激元激发被引量:2
2014年
基于含时密度泛函理论,研究了C60富勒烯二聚物的等离激元激发.当两个C60分子靠近,分子之间的间隙较大,通过电容性相互作用时,二聚物的低能等离激元共振模式随着间隙的减小发生红移.进一步减小间隙时,由于电子的隧穿,C60富勒烯二聚物的等离激元共振模式发生了改变,长程电荷转移激发模式形成.与金属纳米结构二聚物不同,当再继续减小间隙时,长程电荷转移激发模式没有发生蓝移,而是继续红移.在可见光范围内,C60富勒烯二聚物有很强的吸收光谱.
尹海峰张红岳莉
关键词:等离激元含时密度泛函理论
C掺杂锐钛矿TiO_2电子结构和光学性质的第一性原理计算被引量:3
2011年
基于第一性原理,计算了碳掺杂锐钛矿相TiO_2的电子结构和光学性质.计算结果表明,纯TiO_2的晶格参数与实验值以及其它的理论结果符合的很好;碳掺杂TiO_2的带隙间出现了三个孤立的非纯态;掺杂TiO_2的带隙和结构参数随着掺杂碳的含量和分布方式变化;碳掺杂TiO_2可以吸收波长更长的太阳光,有助于提高TiO_2的可见光催化活性.
朱博栾翠星朱俊郝彦军雷爱兵
关键词:光催化活性带隙第一性原理
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