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1.
利用耦合簇方法和Dunning等提出的系列相关一致基对PH2自由基的基态结构进行优化, 并使用优选出的cc-pV5Z基组对其进行频率计算. 结果表明,平衡核间距RP—H=0.14185 nm, 键角αHPH=91.8624°, 离解能De(HP—H)=3.483 eV, 对称伸缩振动频率ν1a1)=2399.9781 cm-1, 弯曲振动频率ν2a1)=1128.4213 cm-1,反对称伸缩振动频率ν3b2)=2407.8374 cm-1. 在此基础上采用多体项展式理论导出了PH2自由基的解析势能函数, 其等值势能图准确再现了PH2自由基分子的平衡结构特征和动力学特征. 关键词: 2自由基')" href="#">PH2自由基 多体项展式理论 解析势能函数  相似文献   

2.
运用单双迭代三重激发耦合簇理论和相关一致五重基对SiH2的基态结构进行了优化, 并在优化结构的基础上进行了离解能和振动频率的计算. 结果表明: SiH2的基态为C2v结构, 平衡核间距RSi—H= 0.15163 nm, H—Si—H键的键角α=92.363°, 离解能De(HSi—H)=3.2735 eV, 频率ν1a1)=1020.0095 cm-1, ν2a1)=2074.8742 cm-1, ν3a1)=2076.4762 cm-1. 这些结果与实验值均较为相符. 对H2的基态使用优选出的cc-pV6Z基组、对SiH的基态使用优选出的aug-cc-pV5Z基组进行几何构型与谐振频率的计算并进行单点能扫描, 且将扫描结果拟合成了解析的Murrell-Sorbie函数. 与实验结果及其他理论计算结果的比较表明, 本文关于SiH自由基光谱常数(De,Re, ωe, Be, αeωeχe)的计算结果达到了很高的精度. 采用多体项展式理论导出了SiH2C2v, X1A1)自由基的解析势能函数, 其等值势能图准确再现了它的离解能和平衡结构特征. 同时还给出了SiH2(C2v, X1A1)自由基对称伸缩振动等值势能图中存在的两个对称鞍点, 对应于SiH+H→SiH2反应, 势垒高度为0.5084 eV. 关键词: 2')" href="#">SiH2 Murrell-Sorbie函数 多体项展式理论 解析势能函数  相似文献   

3.
HNO分子基态的结构与解析势能函数研究   总被引:1,自引:0,他引:1       下载免费PDF全文
赵俊  曾晖  朱正和 《物理学报》2011,60(11):113102-113102
应用群论及原子分子反应静力学的方法, 导出了HNO分子基态电子态和合理的离解极限.利用优选出的密度泛函理论B3LYP方法结合6-311G **优化计算了HNO分子基态的平衡结构和谐振频率.计算结果表明基态HNO分子稳定态为CS构型,电子组态为X1A',平衡核间距分别为RH-N=0.1065 nm,RN-O=0.1200 nm,键角∠H-N-O=108.60°,离解能De=15.379 eV.基态简正振动频率分别为:弯曲振动频率ν1=1575.6351 cm-1,对称伸缩振动频率ν2=1673.2890 cm-1,反对称伸缩振动频率ν3=2837.7856 cm-1.在此基础上,应用多体项展式理论导出了基态HNO分子的全空间解析势能函数,该势能函数等值势能图准确再现了HNO分子平衡结构和离解能. 关键词: 势能函数 光谱常数 密度泛函方法  相似文献   

4.
谢安东  谢晶  周玲玲  伍冬兰  阮文  罗文浪 《物理学报》2015,64(6):63301-063301
对铀原子和氮原子分别使用相对论有效原子实势和6-311+G(d)基组, 采用优选的密度泛函B3P86方法, 研究了铀本身产生自辐射场(-0.005–0.005 a.u.)作用下UN2基态分子的能隙Eg和谐振频率ν. 结果表明: UN2分子在自辐射场中反对称伸缩振动频率ν3(σg)和对称伸缩振动频率σ1(σg)与实验值1051.1 cm-1和1008.3 cm-1 基本符合; Eg随自辐射场场强的增大而趋于减少, 占据轨道的电子容易被激发至空轨道而形成激发态; UN2分子在自辐射场中趋于不稳定, N2, O2等更容易扩散到表面内层而腐蚀铀表面, 加剧了铀在自辐射场中的腐蚀.  相似文献   

5.
BH2和AlH2分子的结构及其解析势能函数   总被引:1,自引:0,他引:1       下载免费PDF全文
运用二次组态相关(QCISD)方法,分别选用6-311++G(3df,3pd)和D95(3df,3pd)基组,对BH2和AlH2分子的结构进行了优化计算,得到BH2分子的稳态结构为C2v构型,电子态为2A1、平衡核间距RBH=0.1187nm、键角∠HBH=128.791°、离解能De=3.65eV、基态振动频率ν1(a1)=1020.103cm-12(a1)=2598.144cm-13(b2)=2759.304cm-1.AlH2分子的稳态结构也为C2v构型,电子态为2A1、平衡核间距RAlH=0.1592nm、键角∠HAlH=118.095°、离解能De=2.27eV、基态振动频率ν1(a1)=780.81cm-12(a1)=1880.81cm-1,ν3(b2)=1910.46cm-1.采用多体项展式理论推导了基态BH2和AlH2分子的解析势能函数,其等值势能图准确再现了BH2和AlH2分子的结构特征及其势阱深度与位置.分析讨论势能面的静态特征时得到BH+H→BH2反应中存在鞍点,活化能为150.204kJ/mol;AlH+H→AlH2反应中也存在鞍点,活化能为54.8064kJ/mol. 关键词: 2')" href="#">BH2 2')" href="#">AlH2 Murrell-Sorbie函数 多体项展式理论 解析势能函数  相似文献   

6.
运用Gaussian 03程序包中的单双迭代三重激发耦合簇理论和相关一致五重基优化了AsH2的基态结构,并在优化结构的基础上计算了它的离解能和振动频率. 结果表明:AsH2基态的平衡构型具有C2v对称性,键长RAs-H=01508 nm,键角∠HAsH=912231°,离解能De(HAs-H)=28795 eV,振动频率ν 关键词: 2')" href="#">AsH2 Murrell-Sorbie函数 多体项展式理论 解析势能函数  相似文献   

7.
赵俊  程新路  杨向东  朱正和 《物理学报》2009,58(8):5280-5284
运用Gaussian03软件包,采用密度泛函理论中的B3P86 方法,结合6-311++G**(3df,3pd) 基组对基态SiF2分子的平衡电子结构和谐振频率进行了优化计算,得到了其稳定结构为C2v构型.SiF2基态电子态为X1A1,平衡核间距RSi—F=0.1061 nm,键角αF—Si—F=100.6762°,离解能De=13.8 eV.应用多体项展式理论推导了基态SiF2分子的解析势能函数,其等值势能图准确地再现了SiF2分子的平衡构型特征和能量变化. 关键词: 2')" href="#">SiF2 Murrell-Sorbie函数 多体项展式理论  相似文献   

8.
在B3P86/cc-PVTZ水平上,对N2O异构体进行优化计算,得出N2O基态的单重态能量最低,其稳定构型为Cv构型,平衡核间距R1=0.1121nm,R2=0.1177nm,α=180°,能量为-185.1188a.u.同时计算出基态的简正振动频率ω1(Π)=601.5010 cm关键词: 异构体 多体项展式理论 解析势能函数  相似文献   

9.
NiH2分子的结构及其势能函数   总被引:9,自引:3,他引:6  
应用群论及原子分子反应静力学方法推导了NiH2分子基态的电子态及其离解极限,在MP2/6-311G水平上,优化出NiH2(3Δg)分子稳定构型为D∞h,其平衡核间距Re=0.157 3 nm、∠HNiH=180.00°,同时计算出振动频率:对称伸缩振动频率ν1=2 000 cm-1,弯曲振动频率ν2=721 cm-1和反对称伸缩振动频率ν3=1 875 cm-1.在此基础上,使用多体项展式理论方法,导出了基态NiH2分子的全空间解析势能函数,该势能函数准确地再现了NiH2(D∞h)平衡结构.  相似文献   

10.
应用群论及原子分子反应静力学方法推导Si分子的电子态及其离解极限,在B3P86/CC-PVTZ水平上,对Si3分子基态进行优化计算,得出Si3基态的单重态能量最低,其稳定构性为的C2V构型,平衡核间距Re=0.2176nm、∠213=79.7°,能量为-869.2057a.u..同时计算出基态的简正振动频率:对称伸缩振动频率ν(B2)=547.6446cm-1,弯曲振动频率ν(A1)=185.6100cm-1和反对称伸缩振动频率ν(A1)=559.6090cm-1.在此基础上,使用多体项展式理论方法,导出了基态Si3分子的全空间解析势能函数,该势能函数准确再现了Si3(C2V)平衡结构.  相似文献   

11.
应用群论及原子分子反应静力学方法推导了SiO2分子的电子态及其离解极限,采用B3P86方法,在6-311G**水平上,优化出SiO2基态分子稳定构型为单重态的C2V构型,其平衡核间距Re=RSi—O=0.1587 nm,∠OSiO=111.2°,能量为-440.4392 a.u..同时计算出基态的简正振动频率:对称伸缩振动频率ν(B2)=945.4cm-1,弯曲振动频率ν(A1)=273.5 cm-1和反对称伸缩振动频率ν(A1)=1362.9cm-1.在此基础上,使用多体项展式理论方法,导出了基态SiO2分子的全空间解析势能函数,该势能函数准确再现了SiO2(C2V)平衡结构.  相似文献   

12.
曾晖  赵俊 《中国物理 B》2012,(7):579-584
In this paper, the energy, equilibrium geometry, and harmonic frequency of the ground electronic state of PO2 are computed using the B3LYP, B3P86, CCSD(T), and QCISD(T) methods in conjunction with the 6-311++G(3df, 3pd) and cc-pVTZ basis sets. A comparison between the computational results and the experimental values indicates that the B3P86/6-311++G(3df, 3pd) method can give better energy calculation results for the PO 2 molecule. It is shown that the ground state of the PO2 molecule has C2v symmetry and its ground electronic state is X2 A1 . The equilibrium parameters of the structure are R P O = 0.1465 nm, ∠OPO = 134.96°, and the dissociation energy is Ed = 19.218 eV. The bent vibrational frequency ν 1 = 386 cm-1 , symmetric stretching frequency ν 2 = 1095 cm-1 , and asymmetric stretching frequency ν 3 = 1333 cm-1 are obtained. On the basis of atomic and molecular reaction statics, a reasonable dissociation limit for the ground state of the PO2 molecule is determined. Then the analytic potential energy function of the PO2 molecule is derived using many-body expansion theory. The potential curves correctly reproduce the configurations and the dissociation energy for the PO2 molecule.  相似文献   

13.
基态UC2分子的结构和势能函数   总被引:5,自引:0,他引:5  
采用密度泛函理论 (DFT)的B3LYP方法和相对论有效原子实势理论模型 (RECP) ,对UC2 分子可能的结构进行优化计算 ,得到UC2 分子稳定构型为角形C -U -C(C2v) ;由微观可逆性原理 ,判断了UC2 分子的离解极限 ;并且导出了基态UC2 分子 (X 5B1)的多体项展式势能函数 ,其势能面等值图展现了C -U -C(C2v)稳定结构 ;根据势能面等值图 ,讨论了C +UC(X 3 П)反应和U +C2 (X 1∑+ g)反应的势能面静态特征  相似文献   

14.
Zeng Hui  Zhao Jun 《中国物理 B》2012,21(7):78202-078202
In this paper, the energy, the equilibrium geometry, and the harmonic frequency of the ground electronic state of PO2 are computed using B3LYP, B3P86, CCSD(T), and QCISD(T) methods in conjunction with 6-311++G(3df, 3pd) and cc-pVTZ basis sets. A comparison between the computational results and the experimental values indicates that the B3P86/6-311++G(3df, 3pd) method can give better energy calculation results for the PO2 molecule. It is shown that the ground state of the PO2 molecule has C2v symmetry and its ground electronic state is X2A1. The equilibrium parameters of the structure are RP-O=0.1465 nm, d=19.218 eV. The bent vibrational frequency ν1=386 cm-1, the symmetric stretching frequency ν2=1095 cm-1, and the asymmetric stretching frequency ν3=1333 cm-1 are obtained. On the basis of atomic and molecular reaction statics, the reasonable dissociation limit for the ground state of the PO2 molecule is determined. Then the analytic potential energy function of the PO2 molecule is first derived by using the many-body expansion theory. The potential curves correctly reproduce the configurations and the dissociation energy for the PO2 molecule.  相似文献   

15.
根据群论及原子分子反应静力学的有关原理,推导了PS基态分子电子态及其合理的离解极限.采用Gaussian 03软件中的密度泛函理论B3LYP和B3P86结合6-311++G(3df,3pd)、6-311++G、6-311G(3df,3pd)、cc-p VTZ和D95基组,对PS分子基态平衡结构和谐振频率进行了计算.通过比较计算结果,发现B3P86方法结合cc-p VTZ基组计算所得结果与实验值最接近.在该水平下对PS分子的基态进行了单点势能扫描计算,利用正规方程组拟合三参数的Murrell-Sorbie函数和修正的Murrell-Sorbie+C6函数,得到了基态PS分子完整的势能函数与相应的光谱常数ωe、ωexe、Be和αe的值.计算结果表明,利用三参数的Murrell-Sorbie函数计算所得的光谱常数与实验数据吻合得更好.  相似文献   

16.
基态TiH2分子的结构与分析势能函数   总被引:4,自引:0,他引:4  
用密度泛函理论的B3lyp方法,Ti原子采用相对论有效实势(LanL2DZ)收缩价基函数,氢原子采用6-311 g**全电子基函数,对TiH2体系的结构进行优化计算.得到TiH2分子最稳态为C2v构型,电子状态为(C2v(X)3A2),平衡核间距,RTi-H=0.1789 nm,键角∠HTiH =123.365°,离解能:De=5.54216 eV.基态简正振动频υ(A1)=485.4150 cm-1,υ(B2)=1507.6533 cm-1,υ(A1)=1580.2361 cm-1.由微观过程的可逆性原理分析了分子的可能离解极限,并用多体项展式理论方法分别导出基态TiH2分子的势能函数,其等值势能面图准确地再现了TiH2分子的结构特征和离解能.由此讨论了TiH2分子反应的势能面静态特征.  相似文献   

17.
伍冬兰  谢安东  余晓光  万慧军 《中国物理 B》2012,21(4):43103-043103
The equilibrium structure of flue gas SO2 is optimized using the density functional theory (DFT)/B3P86 method and CC-PV5Z basis. The result shows that it has a bent (C2v, X1A1) ground state structure with an angle of 119.1184°. The vibronic frequencies and the force constants are also calculated. Based on the principles of atomic and molecular reaction statics (AMIIS), the possible electronic states and reasonable dissociation limits for the ground state of SO2 molecule are determined. The potential functions of SO and 02 are fitted by the modified Murrell-Sorbie+c6 (M-S+c6) potential function and the fitted parameters, the force constants and the spectroscopic constants are obtained, which are all close to the experimental values. The analytic potential energy function of the SO2 (X1A1) molecule is derived using the many-body expansion theory. The contour liues are constructed, which show the static properties of SO2 (XIA1), such as the equilibrium structure, the lowest energies, the most possible reaction channel, etc.  相似文献   

18.
阎世英  朱正和 《中国物理》2004,13(12):2053-2057
Density functional method (DFT) (B3p86) of Gaussian98 has been used to optimize the structure of the Tc_2 molecule. The result shows that the ground state for Tc_2 molecule is an 11-multiple state and its electronic configuration is {}^{11}Σ_g^-, which shows the spin polarization effect of Tc_2 molecule of a transition metal element for the first time. Meanwhile, we have not found any spin pollution because the wavefunction of the ground state does not mingle with wavefunctions of higher energy states. So, that the ground state for Tc_2 molecule is an 11-multiple state is indicative of the spin polarization effect of Tc_2 molecule of a transition metal element: that is, there exist 10 parallel spin electrons. The non-conjugated electron is greatest in number. These electrons occupy different spacious tracks, so that the energy of Tc_2 molecule is minimized. It can be concluded that the effect of parallel spin of the Tc_2 molecule is larger than the effect of the conjugated molecule, which is obviously related to the effect of electron d delocalization. In addition, the Murrell--Sorbie potential functions with the parameters for the ground state {}^{11}Σ_g^- and other states of Tc_2 molecule are derived. Dissociation energy D_e for the ground state of T_{c2} molecule is 2.266eV, equilibrium bond length R_e is 0.2841nm, vibration frequency ω_e is 178.52cm^{-1}. Its force constants f_2, f_3, and f_4 are 0.9200aJ·nm^{-2}, --3.5700aJ·nm^{-3}, 11.2748aJ·nm^{-4} respectively. The other spectroscopic data for the ground state of Tc_2 molecule ω_eχ_e, B_e, α_e are 0.5523cm^{-1}, 0.0426cm^{-1}, 1.6331×10^{-4}cm^{-1} respectively.  相似文献   

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