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从密度泛函理论为基础的第一性原理出发,运用全势能线性缀加平面波(FLAPW)方法,对氚衰变后氦在合金中的占位以及LaNi5He晶体结构进行了理论计算,并系统给出了氦在间隙间的迁移曲线.结果表明,氦原子在十二面体(1b)格位最稳定,并且氦从6m格位向1b格位迁移不存在势垒,而从2d格位向1b格位迁移则需越过1.55eV高的势垒.另外,氦从12n格位穿过12o格位最后到达6m格位也无明显势垒存在,并且处于4h格位之间的氦原子可以自由迁移,而相应12n格位之间的直接迁移则需跨越13.6eV高的势垒.最后还计算给出了氚衰变后合金的态密度、电子密度以及势能分布图,并与相应的LaNi5H结构作了详细比较.
关键词:
全势能线性缀加平面波(FLAPW)
5He')" href="#">LaNi5He
态密度
扩散 相似文献
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Geometries,stabilities, and electronic properties analysis in In_nNi~((0,±1)) clusters: Molecular modeling and DFT calculations 下载免费PDF全文
Density functional theory(DFT) with the B3 LYP method and the SDD basis set is selected to investigate In_nNi,In_nNi~-, and In_nNi~+ (n = 1–14) clusters. For neutral and charged systems, several isomers and different multiplicities are studied with the aim to confirm the most stable structures. The structural evolution of neutral, cationic, and anionic In_nNi clusters, which favors the three-dimensional structures for n = 3–14. The main configurations of the In_nNi isomers are not affected by adding or removing an electron, the order of their stabilities is also nearly not affected. The obtained binding energy exhibits that the Ni-doped In_(13) cluster is the most stable species of all different sized clusters. The calculated fragmentation energy and the second-order energy difference as a function of the cluster size exhibit a pronounced even–odd alternation phenomenon. The electronic properties including energy gap(E_g), adiabatic electron affinity(AEA), vertical electron detachment energy(VDE), adiabatic ionization potential energy(AIP), and vertical ionization potential energy(VIP) are studied. The total magnetic moments show that the different magnetic moments depend on the number of the In atoms for charged In_nNi. Additionally, the natural population analysis of In_nNi~((0,±1)clusters is also discussed. 相似文献
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在全电子水平上,采用广义梯度近似密度泛函理论和全势能线性缀加平面波方法并结合二维立方拟合方法,对LaNi3.75Al1.25合金的晶体结构与弹性性质进行了理论研究.计算结果给出合金的晶格常数a=b=0.5137 nm,c=0.4018 nm,Al原子在晶胞中的微观分布为同时占据部分3g和2c等价格位,弹性常数C11+C12=281.2,C13=82.3,C33=227.3,以及体弹性模量B=124.5、切变模量G=68.2 GPa.还对态密度、能带结构和电荷密度进行了计算分析,并给出材料LaNi3.75Al1.25的电子线性比热系数23.45 mJ/molK2.
关键词:
3.75Al1.25')" href="#">LaNi3.75Al1.25
储氢合金
全势能线性缀加平面波
弹性常数 相似文献
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从密度泛函理论为基础的第一性原理出发,运用全势能线性缀加平面波(FLAPW)方法,对氚衰变后氦在合金中的占位以及LaNiHe晶体结构进行了理论计算,并系统给出了氦在间隙间的迁移曲线.结果表明,氦原子在十二面体(1 b)格位最稳定,并且氦从6m格位向1 b格位迁移不存在势垒,而从2d格位向1 b格位迁移则需越过1.55 eV高的势垒.另外,氦从12n格位穿过12o格位最后到达6m格位也无明显势垒存在,并且处于4h格位之间的氦原子可以自由迁移,而相应12n格位之间的直接迁移则需跨越13.6 eV高的势垒.最后还计算给出了氚衰变后合金的态密度、电子密度以及势能分布图,并与相应的LaNi5H结构作了详细比较. 相似文献
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在全电子水平上,采用广义梯度近似密度泛函理论和全势能线性缀加平面波方法并结合二维立方拟合方法,对LaNi3.75Al1.25合金的晶体结构与弹性性质进行了理论研究.计算结果给出合金的晶格常数a=b=0.5137 nm,c=0.4018 nm,Al原子在晶胞中的微观分布为同时占据部分3g和2c等价格位,弹性常数C11+C12=281.2,C13=82.3,C33=227.3,以及体弹性模量B=124.5、切变模量G=68.2 GPa.还对态密度、能带结构和电荷密度进行了计算分析,并给出材料LaNi3.75Al1.25的电子线性比热系数23.45 mJ/molK2. 相似文献
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采用SAC/SAC-CI方法在CC-PV5Z基组下, 计算研究了He2+、He2++的基态及低激发态的分子特性, 给出了其基态和一些激发态的势能函数和光谱数据(Be、αe、ωe和ωeχe). 从群论出发推导了相应状态的离解极限;与已有实验结果的He2+(X2Σu+)相比, 计算结果令人满意. 还计算了激发态2Πu、4Σu+和4Πg的结构与光谱数据. 对于He2++, 计算的九个电子态中只有三个态(X1Σg+、1Σg+和1Σu+)属束缚态, 并得到了其光谱常数. 用价键理论模型的不相交规则对He2++基态的势能曲线极大点产生的原因做了较好的分析. 相似文献
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First-principles calculations of structure and elasticity of hydrous fayalite under high pressure 下载免费PDF全文
The structures,elasticities,sound velocities,and electronic properties of anhydrous and hydrous fayalite(Fe_2SiO_4and Fe_(1.75)H_(0.5)SiO_4)under high pressure have been investigated by means of the density functional theory within the generalized gradient approximation(GGA)with the on-site Coulomb energy being taken into account(GGA+U).The optimized results show that H atoms prefer to substitute Fe atoms in the Fe1 site.Compared with the anhydrous fayalite Fe_2SiO_4,the mass density,elastic moduli,and sound velocities of Fe_(1.75)H_(0.5)SiO_4 slightly decrease.According to our data,adding 2.3 wt%water into fayalite leads to reductions of compressional and shear wave velocities(VPand VS)by3.4%–7.5%and 0.3%–3.4%at pressures from 0 GPa to 25 GPa,respectively,which are basically in agreement with the2%–5%reductions of sound velocity obtained by the experimental measurement in the low velocity zones(LVZ).Based on the electronic structure,the valence and conduction bands are slightly broader for hydrous fayalite.However,hydrous fayalite keeps the insulation characteristics under the pressures up to 30 GPa,which indicates that hydration has little effect on its electronic structure. 相似文献
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