Abstract:Ab initio calculations (LCAO–MO–SCF) are performed on a series of valence levels of the molecules CH and NH+. Correlation energies are estimated semiempirically from corresponding atomic data. Close agreement with experiment is found for known states for a series of molecular properties such as equilibrium internuclear distances, vibration frequencies, term values, and dissociation energies. A low-lying Σ4− state in CH is calculated to lie 7500 cm−1 above the X 2Π state. No observable quartet transition could … Show more
“…Because of the XH bonding character of the lo MO, one expects a larger r e value compared with the lowest a 4y,-state. Accordingly the present MRD-CI study predicts an elongation of c. 0.8 a o with respect to the lowest quartet state, while similar increases can be estimated from figure 2 of [39] containing results for the CH radical. This second 4y-state correlates with the 5S u (nsnp a) atomic state of C and Si respectively, for which the excitation energy relative to the X apg state [22] is nearly the same in both systems (that is 4-18 eV in C and 4.13 eV in Si).…”
Section: Comparison Between Sill and The Isovalent Ph + Ch And Nh + mentioning
confidence: 63%
“…In the case of Sill the MRD-CI calculations place the 2 4E-state 5.55 eV above the ground state, or roughly 1.40 eV below the Si (sSu) limit. In the case of CH only the theoretical study of Liu and Verhaegen [39] is available for this state, according to which its energy is computed to be 0.90 eV greater than that of its dissociation limit; in this connection it should be noted, however, that these authors have expressed the opinion that this state has been somewhat less satisfactorily described than the other low-lying species. All in all it at least seems likely that the energy relationships between the bound 2 4E-molecular state and its dissociation products is quite different in Sill than in CH.…”
Section: Comparison Between Sill and The Isovalent Ph + Ch And Nh + mentioning
Potential curves and other properties of the ground and excited states of Sill are calculated at close to full CI accuracy in DZP AO basis sets including f functions. The C 2N+ state of this system is shown to correspond to a second potential minimum of the B 2E+ species which occurs because of an avoided crossing with a dissociative state of the same symmetry. The D 2A and E 2)2+ states are assigned as members of Rydberg series involving upper orbitals of d8 and do symmetry respectively. In addition, a number of quartet states have been computed including the qI and two 4E-species which have apparently not yet been characterized experimentally. The 4H state is found to be strongly repulsive, causing predissociation of the 4s and 4p members of the lowest Rydberg series ; this observation is consistent with the fact that transitions to such upper states have yet to be observed experimentally. Computed spectroscopic constants, dipole and transition moments and dissociation energies are all found to agree quite well with ekperiment wherever comparison is possible, including results for spin-orbit constants as a function of vibrational level in the X 2IIr ground state. Comparison is also made with results for the isovalent systems PH +, CH and NH ÷ at various levels and it is noted that NH + exhibits a number of unusual features because of the relatively high value of the nitrogen atom IP.
“…Because of the XH bonding character of the lo MO, one expects a larger r e value compared with the lowest a 4y,-state. Accordingly the present MRD-CI study predicts an elongation of c. 0.8 a o with respect to the lowest quartet state, while similar increases can be estimated from figure 2 of [39] containing results for the CH radical. This second 4y-state correlates with the 5S u (nsnp a) atomic state of C and Si respectively, for which the excitation energy relative to the X apg state [22] is nearly the same in both systems (that is 4-18 eV in C and 4.13 eV in Si).…”
Section: Comparison Between Sill and The Isovalent Ph + Ch And Nh + mentioning
confidence: 63%
“…In the case of Sill the MRD-CI calculations place the 2 4E-state 5.55 eV above the ground state, or roughly 1.40 eV below the Si (sSu) limit. In the case of CH only the theoretical study of Liu and Verhaegen [39] is available for this state, according to which its energy is computed to be 0.90 eV greater than that of its dissociation limit; in this connection it should be noted, however, that these authors have expressed the opinion that this state has been somewhat less satisfactorily described than the other low-lying species. All in all it at least seems likely that the energy relationships between the bound 2 4E-molecular state and its dissociation products is quite different in Sill than in CH.…”
Section: Comparison Between Sill and The Isovalent Ph + Ch And Nh + mentioning
Potential curves and other properties of the ground and excited states of Sill are calculated at close to full CI accuracy in DZP AO basis sets including f functions. The C 2N+ state of this system is shown to correspond to a second potential minimum of the B 2E+ species which occurs because of an avoided crossing with a dissociative state of the same symmetry. The D 2A and E 2)2+ states are assigned as members of Rydberg series involving upper orbitals of d8 and do symmetry respectively. In addition, a number of quartet states have been computed including the qI and two 4E-species which have apparently not yet been characterized experimentally. The 4H state is found to be strongly repulsive, causing predissociation of the 4s and 4p members of the lowest Rydberg series ; this observation is consistent with the fact that transitions to such upper states have yet to be observed experimentally. Computed spectroscopic constants, dipole and transition moments and dissociation energies are all found to agree quite well with ekperiment wherever comparison is possible, including results for spin-orbit constants as a function of vibrational level in the X 2IIr ground state. Comparison is also made with results for the isovalent systems PH +, CH and NH ÷ at various levels and it is noted that NH + exhibits a number of unusual features because of the relatively high value of the nitrogen atom IP.
“…The comparison of total ionization cross sections along an isoelectronic sequence relies on the Thomson's classical scaling law (Thomson 1912), which predicts that the total cross sections scale according to the inverse of the square of the corresponding ionization threshold energy I i (eV). The energy threshold is 10.6eV (Liu and Verhaegen 1970) for CH that is about two times lower than the present 20eV for NH + . Consequently, the total ionization cross section for CH should be about four times larger than the one of NH + and not only two times.…”
Section: Ionizationmentioning
confidence: 86%
“…It can be concluded from the present study that the comparison of the two isoelectronic molecular species is not successful and that the classical formula is inappropriate for molecular ions. Differences among the potential energy diagrams for CH and for NH + which have been pointed out by Liu and Verhaegen (1970) may explain such a discrepancy.…”
To cite this version:J Lecointre, J J Jureta, P Defrance, Kingdom. Electron-impact dissociation and ionization of NH+: formation of N+ and N2+. Journal of Physics B: Atomic, Molecular and Optical Physics, IOP Publishing, 2010, 43 (10)
“…When the nonorthogonality is treated correctly, E is obtained by diagonalizing HFJ defined as 1 2 (17) where S p p is the overlap matrix element between reference configurations P and P' . While eq 17 performs less well than eq 16 in practice, the effective Hamiltonian in eq 17 does yield a better eigenvector since it includes the correlation correction.…”
We present and test a computationally economical scheme for obtaining dynamical correlation energy corrections for complete active space self-consistent field (CASSCF) wave functions. The method relies on the decomposition of the chemical system into "fragments". By use of a localized orbital description any CASSCF wave function can be transformed into a classical valence bond expansion. The advantage of the classical valence bond expansion is that the wave function takes the form of a superposition of fragment covalent and ionic states. The dynamic correlation energy is evaluated, using a density functional method, for each fragment state and added to the total energy according to an "atoms-in-molecules" type formula.The method is tested through application to bond dissociation in HZ and LiH and also to the evaluation of barrier heights for the reactions C1+ HC1-HC1+ C1 and CH3 + C& -C& + CH3 and the Diels-Alder reaction between ethene and butadiene.
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