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1.
The potential energy curves have been investigated for the 10 lowest quartet electronic states in the 2s+1Λ± representation below 30,000 cm?1 of the molecule CrCl via CASSCF and MRCI (singly and doubly excitation with Davidson correction) calculations. The harmonic frequency ωe, the internuclear distance re, the rotational constant Be, the electronic energy with respect to the ground state Te, and the permanent dipole moment μ have been calculated. By using the canonical functions approach, the eigenvalues Ev, the rotational constant Bv, and the abscissas of the turning points rmin and rmax have been calculated for the considered electronic states up to the vibrational level v = 19. Seven electronic states have been studied here theoretically for the first time. The comparison of these values to the theoretical results available in the literature shows a good agreement. © 2010 Wiley Periodicals, Inc. Int J Quantum Chem, 2011  相似文献   

2.
Theoretical investigation of the 18 lowest electronic states of the molecule ScI in the representation 2S+1Λ(±) has been performed via CASSCF and MRCI (single and double excitation with Davidson correction) calculations. To the best of our knowledge these calculated electronic states are the first ones from ab initio methods. Thirteen electronic states between 4,500 cm?1 and 21,000 cm?1 have been studied for the first time and have not yet been observed experimentally. The harmonic frequency ωe, the internuclear distance Re, the electronic transition energy with respect to the ground state Te, and the rotational constant Be have been calculated for the considered electronic states. By using the canonical functions approach the eigenvalues Eυ and the rotational constants Bυ have also been calculated for the six lowest‐lying electronic states. The comparison of these results with the theoretical and the experimental data available in the literature shows a good agreement. © 2008 Wiley Periodicals, Inc. Int J Quantum Chem, 2009  相似文献   

3.
The potential energy curves have been investigated for the 13 lowest sextet electronic states in the representation below 53,000 cm?1 of the molecule CrCl via CASSCF and MRCI (single and double excitation with Davidson correction) calculations. The harmonic frequency ωe, the internuclear distance re, the rotational constant Be, the electronic energy with respect to the ground state Te, and the permanent dipole moment μ have been calculated. By using the canonical functions approach, the eigenvalues Ev, the rotational constant Bv, and the abscissas of the turning points rmin and rmax have been calculated for the considered electronic states up to the vibrational level v = 16. Nine electronic states have been studied theoretically here for the first time. The comparison of these values with the theoretical and experimental results available in the literature shows a good agreement. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2012  相似文献   

4.
Using an ab initio method, the potential energy has been calculated for the 29 lowest molecular states of symmetries 2Σ+, 2Π, 2Δ for the molecular ion RbH+. The calculation is based on nonempirical pseudopotentials and parameterized ?‐dependent polarization potentials. Gaussian basis sets have been used for both atoms. The spectroscopic constants for 18 electronic sates have been calculated by fitting the calculated energy values to a polynomial in terms of the internuclear distance R. Through the canonical functions approach the eigenvalue Ev, the abscissas of the corresponding turning points (Rmin and Rmax) and the rotational constants Bv have been calculated up to 24 vibrational levels for the considered bound states. The comparison of the present results with those available in literature shows a very good agreement. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010  相似文献   

5.
By using CASSCF/MRCI methods, theoretical molecular calculations have been performed for 12 electronic states for AlBr molecule and 12 electronic states for AlI molecule in the representation 2s+1Λ (neglecting spin‐orbit effects). Calculated potential energy curves are displayed. Spectroscopic constants including the harmonic vibrational wave number ωe, the electronic energy Te referred to the ground state and the equilibrium internuclear distance Re are predicted for these singlet and triplet electronic states for both AlBr and AlI molecules. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010  相似文献   

6.
Using an ab initio method the potential energy has been calculated for the 25 lowest molecular states of symmetries 2Σ+, 2Π, 2Δ for the molecular ion KH+. The calculation is based on nonempirical pseudopotentials and parameterized -dependent polarization potentials. Gaussian basis sets have been used for both atoms. The spectroscopic constants for 18 electronic sates have been calculated by fitting the calculated energy values to a polynomial in terms of the internuclear distance R. Through the canonical functions approach the eigenvalue Ev, the abscissas of the corresponding turning points (Rmin and Rmax) and the rotational constants Bv have been calculated up to 24 vibrational levels for the considered bound states. The comparison of the present results with those available in literature shows a very good agreement.  相似文献   

7.
The potential energy curves have been investigated for the 12 lowest sextet electronic states in the 2s+1Λ(±)2s+1Λ(±) representation below 53,000 cm−1 of the molecule CrF via CASSCF and MRCI (single and double excitation with Davidson correction) calculations. Seven electronic states have been studied theoretically for the first time. The harmonic frequency ωe, the internuclear distance Re, the rotational constant Be, the electronic energy with respect to the ground state Te, and the permanent dipole moment μ have been calculated. By using the canonical functions approach, the eigenvalues Ev, the rotational constant Bv and the abscissas of the turning points Rmin and Rmax have been calculated for the considered electronic states up to the vibrational level v = 39. The comparison of these values to the theoretical and experimental results available in the literature shows a good agreement.  相似文献   

8.
OH自由基的高精度量子化学研究   总被引:6,自引:0,他引:6  
采用内收缩MRCI方法(Internally Contracted Multiconfiguration-Reference Configuration Interaction)研究了OH自由基, 计算得到其基态稳定构型的键长是0.09708 nm, 对应的实验值是0.096966 nm, 第一激发态的键长是0.10137 nm,实验值是0.10121 nm. 同时得到势能曲线PECs (Potential Energy Curve), 再分别由Murrell-Sorbie势能函数拟合计算和POLFIT程序计算得到OH自由基在基态X2Π和第一激发态A2Σ+时的光谱数据:平衡振动频率ωe, 非谐性常数ωeχe以及高阶修正ωeYe, 平衡转动常数Be, 振转耦合系数αe, 解离能D0和垂直跃迁能量ν00. 这些理论计算结果与最新的实验值非常吻合, 精确度比前人也有很大提高. 其中我们计算得到基态OH(X2Π)的解离能D0=35568.86 cm-1, 第一激发态OH (A2Σ+)的解离能D0=18953.93 cm-1, 从第一激发态A2Σ+ (ν=0)到基态X2Π (v=0)的垂直跃迁能ν00=32496.42 cm-1.  相似文献   

9.
The potential energy curves (PECs) of eight low‐lying electronic states (X1Σ+, a3Π, a′3Σ+, d3Δ, e3Σ?, A1Π, I1Σ?, and D1Δ) of the carbon monoxide molecule have been studied by an ab initio quantum chemical method. The calculations have been performed using the complete active space self‐consistent field method, which is followed by the valence internally contracted multireference configuration interaction (MRCI) approach in combination with the correlation‐consistent aug‐cc‐pV5Z basis set. The effects on the PECs by the core‐valence correlation and relativistic corrections are included. The way to consider the relativistic corrections is to use the third‐order Douglas–Kroll Hamiltonian approximation at the level of a cc‐pV5Z basis set. Core‐valence correlation corrections are performed using the cc‐pCVQZ basis set. To obtain more reliable results, the PECs determined by the MRCI calculations are corrected for size‐extensivity errors by means of the Davidson modification (MRCI+Q). The spectroscopic parameters (De, Te, Re, ωe, ωexe, ωeye, Be, αe, and γe) of these electronic states are calculated using these PECs. The spectroscopic parameters are compared with those reported in the literature. Using the Breit–Pauli operator, the spin–orbit coupling effect on the spectroscopic parameters is discussed for the a3Π electronic state. With the PECs obtained by the MRCI+Q/aug‐cc‐pV5Z+CV+DK calculations, the complete vibrational states of each electronic state have been determined. The vibrational manifolds have been calculated for each vibrational state of each electronic state. The vibrational level G(ν), inertial rotation constant Bν, and centrifugal distortion constant Dν of the first 20 vibrational states when the rotational quantum number J equals zero are reported and compared with the experimental data. Comparison with the measurements demonstrates that the present spectroscopic parameters and molecular constants determined by the MRCI+Q/aug‐cc‐pV5Z+CV+DK calculations are both reliable and accurate. © 2012 Wiley Periodicals, Inc.  相似文献   

10.
A wide adiabatic study is performed for NaRb molecule, involving 151Σ+ electronic states including the ionic state Na?Rb+, as well as 143Σ+, 1–91,3Π, and 1–51,3Δ states. This investigation is performed using an ab initio approach which involves the effective core potential, the core polarization potential with l‐dependent cut‐off functions. The NaRb system has been treated as a two‐electron system and the full valence configuration interaction is easily achieved. The spectroscopic constants Re, De, Te, ωe, ωexe, Be, and D0 for all these states are derived. We have also computed the vibrational levels as well their spacing for different values of J. In addition, permanent and transition dipole moments are determined and analyzed. The Dunham coefficients have been used to perform experimental spacing to compare directly with our results. The present calculations on NaRb extend previous theoretical works to numerous electronic excited states in the various symmetries. © 2014 Wiley Periodicals, Inc.  相似文献   

11.
PdYH分子的结构与势能函数   总被引:8,自引:1,他引:7  
倪羽  蒋刚  朱正和  孙颖 《化学学报》2005,63(8):764-768
用密度泛函理论的B3LYP方法, 对钯和钇原子采用SDD收缩价基函数, 氢原子采用6-311++G**全电子基函数, 对PdY和PdYH体系的结构进行优化. 计算表明: PdY分子的几何构型为Cv, 其基态为X2Σ态, 键长R=0.24168 nm, 离解能为De=2.8261 eV, 谐振频率ωe=254.0656 cm-1, 并拟合得到Murrell-Sorbie势能函数; PdYH分子最稳态为Cs构型, 电子组态为1A', 平衡核间距RPdY=0.24281 nm, RYH=0.19824 nm, 键角∠PdYH=116.7157°, 离解能De=5.6146 eV, 基态简正振动频率: 对称伸缩振动频率ν1 (a')=348.2909 cm-1, 弯曲振动频率ν2 (a')=243.3382 cm-1, 反对称伸缩振动频率ν3 (a')=1442.2695 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PdY和PdYH分子的势能函数, 其等值势能面图准确地再现了PdY和PdYH分子的结构特征和离解能, 由此讨论了Pd+Y+H分子反应的势能面静态特征.  相似文献   

12.
The potential energy curves of the molecular ion KRb+ have been investigated for the 60 lowest molecular states of symmetry 2Σ+, 2Π, 2Δ, and Ω = 1/2, 3/2, and 5/2. Using an ab initio method, the calculation has been done in a one active electron approach based on nonempirical pseudopotentials with core valence effects taken into account through parameterized l‐dependent polarization potentials. Using the canonicals functions approach a rovibrational study is done by calculating the eigenvalues Ev, the rotational constants Bv, the centrifugal distortion constants Dv (up to 135 vibrational levels), and the spectroscopic constants ωe and Be for the five electronic states (1)2Σ+, (3)2Σ+, (1)2Π, (1)Ω = 1/2, and (1)Ω = 3/2. No comparison of these values with other results is yet possible because they are given here for the first time. Extensive tables of energy values of Ev, Bv, and Dv are displayed at http://hplasim2.univ‐lyon1.fr/allouche . © 2003 Wiley Periodicals, Inc. Int J Quantum Chem, 2003  相似文献   

13.
Ab initio calculations at SCF and CEPA levels using large Gaussian basis sets have been performed for the two lowest electronic states,X 2 Σ+ andA 2 Π, of HeAr+. Spin-orbit coupling (SOC) effects have been added using a semiempirical treatment. The resulting potential curves for the three statesX,A 1, andA 2 have been used to evaluate molecular constants such as vibrational intervals ΔG(v + 1/2) and rotational constantsB v as well as — by means of a Dunham expansion — equilibrium constants such asR e , ω e ,B e etc. Comparison with the experimental data from UV emission spectroscopy shows that the calculated potential curves are slightly too shallow and have too large equilibrium distances:D e = 242 cm?1 andR e = 2.66 Å compared to the experimental values of 262 cm?1 and 2.585 Å, respectively, for theX 2Σ+ ground state. However, the ab initio calculations yield more bound vibrational levels than observed experimentally and allow for a more complete Dunham analysis, in particular for theA 2 state. The experimental value of 154 cm?1 for the dissociation energyD e of this state is certainly too low; our best estimate is 180±5 cm?1. For theA 1 state our calculations are predictions since this state has not yet been observed experimentally.  相似文献   

14.
The self-consistent-field molecular-orbital method in LCAO (linear combination of atomic orbitals) approximation is applied to the ground and three ionized states of N2 at a number of internuclear distances for the computation of the potential energy curves. In these calculations both the linear coefficients and the screening constants of the atomic orbitals have been optimized. The molecular constants ωe, ωexe, Be, αe, and Re have also been calculated for the above states from the computed potential energy curves. The computed spectral results are compared with the experimental data as well as with the results reported by others from ab initio calculations.  相似文献   

15.
The potential energy curve (PEC) for the ground state of AsP(X1Σ+) has been investigated by the highly accurate valence internally contracted multireference configuration interaction method in the Molpro2008 program package with the correlation consistent basis set. The PEC is fitted to the analytic Murrrell–Sorbie function (M–S function) from which the spectroscopic constants are determined. The present De, Be, αe, ωeχe, Re, and ωe values are of 4.2823 eV, 0.188622 cm?1, 0.000749 cm?1, 1.984427 cm?1, 2.0194 Å, and 598.60 cm?1, respectively. In addition, by numerically solving the radial Schrödinger equation of nuclear motion in the adiabatic approximation, the total of 96 vibration states is predicted when the rotational quantum number J = 0. The complete vibration levels, classical turning points, inertial rotation, and centrifugal distortion constants are reproduced. Comparison has been made with recent theoretical and experimental data. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2012  相似文献   

16.
By using the electronic wave functions obtained from an ab initio calculation, including the spin‐orbit coupling, the electronic transition moments have been investigated for two bound states of symmetry Ω = 1/2 and Ω = 3/2 of the molecular ion KRb+. Based on a canonical functions approach for the determination of the vibrational wave functions, the matrix elements have been calculated for the bound states considered for v = 0, 10, 20 with v′‐ v = 0, 1, 2, …, 6; by using the same canonical approach, the eigenvalues and abscissas of the corresponding turning points (rmin and rmax) have been investigated for these states that obtained from a theoretical ab initio calculation up to v = 105. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2005  相似文献   

17.
The ab initio calculation methods have been used to calculate the spectral and electronic characteristics of difluorocarbene in the ground electronic state (1A1), the lowest-lying singlet (1B1) and triplet (3B1) states. The optimized equilibrium geometries, rotational constants, harmonic vibrational frequencies and energy gaps, electronic charges, dipole moments of these states have been computed with different basis sets. The calculated vibrational frequency of 3B1 state (v2=522 cm?1) and the energy separation (2.26 eV) between 3B1 and 1A1 states are in good agreement with the experimental results (519 cm?1, 2.46 eV respectively). According to the calculations the previous assignment of vibrational symmetries of 1B1 state was corrected, and some experimentally undetermined vibrational frequencies were predicted.  相似文献   

18.
 The ground state and several low-lying excited states of the Mg2 dimer have been studied by means of a combination of the complete-active-space multiconfiguration self-consistent-field (CASSCF)/CAS multireference second-order perturbation theory (CASPT2) method and coupled-cluster with single and double excitations and perturbative contribution of connected triple excitations [CCSD(T)] scheme. Reasonably good agreement with experiment has been obtained for the CCSD(T) ground-state potential curve but the dissociation energy of the only experimentally known A1Σ u + excited state of Mg2 is somewhat overestimated at the CASSCF/CASPT2 level. The spectroscopic constants D e, R e and ωe deduced from the calculated potential curves for other states are also reported. In addition, some spin–orbit matrix elements between the excited singlet and triplet states of Mg2 have been evaluated as a function of internuclear separation. Received: 10 May 2001 / Accepted: 15 August 2001 / Published online: 30 October 2001  相似文献   

19.
Sixteen low-lying electronic states of NaLi are investigated by SCF/valence Cl calculations including core polarization effects by means of an effective potential. Spectroscopic constants are obtained with estimated uncertainties of ΔRe ? 0.01 Å, Δωe ? 0.6 cm?1 and ΔDe ? 80 cm?1. From a comparison of experimental and theoretical G(υ) values, we suggest a ground-state dissociation energy of 7093 ± 5 cm?1. Using our rovibrational energies and recently measured excitation lines, we are able to improve the Te values and dissociation energies of five excited states to an accuracv of ±8 cm?1.  相似文献   

20.
The electronic and rovibrational structure of (1A1) NaH2 + has been investigated using a relativistically-corrected, all-electron coupled-cluster with singles, doubles and perturbative triples (CCSD(T)) ansatz. For the electronic ground state this ansatz yielded equilibrium Na–H bond lengths (R e ) of 2.4208 Å and an equilibrium H–Na–H bond angle (θe) of 17.8°. An analytical potential energy surface (PES) was embedded in the rovibrational Hamiltonian. The PES was constructed using 118 CCSD(T) points and exhibited a residual error of 1.2 cm?1. The rovibrational Hamiltonian was diagonalised using variational techniques. The vibrational and rovibrational eigenvectors were assigned using a configuration weight scheme in terms of normal modes and the Mulliken assignment scheme, respectively. For the ground vibrational state of (1A1) NaH2 +, the vibration-averaged bond lengths 〈R〉 and angle 〈θ〉 were 2.4995 Å and 17.1°, respectively. The ab initio (1A1) NaH2 + PES yielded a dissociation energy (D 0) value of 10.3 kJ mol?1, which is in excellent agreement with the experimental value of 10.3 ± 0.8 kJ mol?1 (Bushnell et al. in J Phys Chem 98:2044, 1994). An analytical dipole moment surface was constructed using 90 CCSD(T) points. Rovibrational spectra of (1A1) NaH2 +, (1A′) NaHD+ and (1A1) NaD2 + for v ≤ 10, J ≤ 5 were constructed using rovibrational transition moment matrix elements calculated in a novel manner that employs the analytical dipole moment surface (DMS). The rovibrational structure of the Na+–H2 v HH = 1 ← v HH = 0 band was calculated and compared to that of Li+–H2.  相似文献   

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