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1982, Soviet Physics Journal
A.P. Ivanov, Physical Foundations of Hydrooptics [in Russian], Nauka i Tekhnika, Minsk (1975). 10. V.E. Zuev, Propagation of Visible and Infrared Waves in the Atmosphere [in Russian], Soy. Radio, Moscow (1970). 11. S.B. Mogil'nitskii, Izv. Vyssh. Uchebn. Zaved., Fiz., No. 11, 117 (1979). PADE FORM OF EFFECTIVE ROTATIONAL MOLECULAR HAMILTONIANS V. N. Bryukhanov, Yu. S. Makushkin, V1. G. Ty~aterev, and V. N. CherepanoV UDC 539.194 Effective rotational molecular Hamiltenians (ERH) are constructed which differ from the traditional representation of the ERH as a power series in the total angular momentum. A Padeform of the ERH is systematically obtained and the nonuniqueness of this form is emphasized. Rapid progress in high and superhigh resolution spectroscopic techniques has led to several questions in the theory of molecular spectra. For example, recent studies of infrared and microwave molecular spectra have shown a very strong dependence of the rotational states on quantum number, and this is difficul~ to interpret with the traditional representation of the effective rotational Hamiltonian as a polynomial in powers of projections of the total angular momentum Jc~. Derivations of other forms of the ERH different from the traditional ones have not appeared in the literature. In the present paper, we use methods previously developed by us to obtain systematically the Pade-form of the ERH and also formulas for some of the spectroscopic constants which appear in one of the possible rational function representations of the ERH.
Internet Electronic Journal of Molecular Design, 2006
Motivation. The problem of the radial matrix elements in the infrared transition vJ v'J' of a diatomic molecule is considered. By using a new expansion in the perturbation theory of the eigenvalue and the eigenfunction of the two considered states in terms of the running number m we derived analytical expressions for the Herman-Wallis coefficients of the rotational factor in the rovibrational matrix elements. The numerical application to the ground states of the molecule HCl shows that the present formulation provides a simple and accurate method for the calculation of the Herman-Wallis coefficients, even for the high order coefficients, without any restriction on the potential function, the operator f(r) and the vibrational levels v and v'. Method. The most important methods used in this investigation are the Rayleigh-Schrödinger perturbation theory and the canonical functions approach. Results. The main results reported in the paper are the determination of the Herman-Wallis coefficients. Conclusions. The method used for the determination of the Herman-Wallis coefficients in this work allows the calculation of these coefficients for any type of potential function and to any order of correction in the perturbation theory. Keywords. Herman-Wallis coefficients for infrared transitions.
Journal of Quantitative Spectroscopy and Radiative Transfer, 1994
The rotational dependence of dipole moments M$" = (YuJJlfl Y,,J) in infrared transitions (tJcto'J') is considered. Analytic theoretical expressions of the Herman-Wallis coefficients for the infrared transitions are investigated by using an unconventional approach of the Rayleigh-Schrijdinger perturbation theory. The rotational factor G$" = M$'/Mg is expressed, in terms of the Bouanich-Herman-Wallis coefficients, by G,,.(m) = 1 + C'm+D'm2+E'm'+... with m = [J'(J' + 1)-J(J + 1)]/2 and J'-J = f 1. The coefficients C', D', and E' are given in terms of the intergrals (@,lfl@,,) and (O,j@,,) where @ stands for the pure-vibrational wavefunction Y', or for one of its successive perturbative corrections go, 9",. .. These expressions are valid for any potential, whether empirical or of the RKR type, and for any operatorf of the form x = (rr,)/r,, x', exp(ax) and others. Numerical application of the present formulation in terms of the Dunham potential in the ground state of CO (for the transitions v = 0, 10, 20 and v'-v < 4) and the ground state of HCI (for the transitions v = 0 and Av < 7) shows the good accuracy.
2005
Computational spectrometry, which implies an interaction between quantum chemistry and analysis of molecular spectra to derive accurate information about molecular properties, is needed for the analysis of the pure rotational and vibration-rotational spectra of HeH+ in four isotopic variants to obtain precise values of equilibrium internuclear distance and force coefficient. For this purpose, we have calculated the electronic energy, rotational and vibrational g factors, the electric dipolar moment, and adiabatic corrections for both He and H atomic centres for internuclear distances over a large range 10-10m [0.3, 10]. Based on these results we have generated radial functions for atomic contributions for gr, g[upsilon], and adiabatic corrections, involving the coefficients sjHe, sjH, tjHe, tjH, ujHe, and ujH of z[thin space]j for 4He1H+ for further spectral analysis.
Chemical Physics Letters, 1990
In majority of publications the spectrum of diatomic molecules in far infrared spectral area is described as a purely quantum phenomenon, and the spectrum in near infrared spectral area is described by means of using a semi-classical approach. In our work an attempt to describe the both spectra from mechanical point of view is presented. The approach is based on accounting of the inertia properties of an interatomic bond. In such approach a potential of interaction between atoms in a molecule is defined by a set of partial differential equations. Good agreement with known experimental data in far infrared spectral area and a qualitative explanation of a thin structure of a resonant peak in the near infrared spectral area is obtained.
Journal of Physics Communications, 2020
Wave functions for terms with the same orbital angular momentum L and spin angular momentum S, but different parents can be written as a linear combination of the pure parentage wave functions. These wavefunctions are important because various spectroscopic quantities e.g. energy and transition probability can be calculated with the help of these wavefunctions. In this study we present 46 wavefunctions of seventeen terms (2P,2D, 2F, 2G, 2H, 2I, 2K, 2L, 4S, 4D, 4F, 4G, 4I,( 2D, 2F, 2G, 2H) are repeated terms, all terms have seniorty number 3 except 2F whose seniorty number is 1) of 4 f 3 6 s 2 configuration of Pr I, with seven parents (1S, 1D, 1G, 1I, 3P, 3F, 3H) belonging to f 2 . Some of the wavefunctions are non-orthogonal as they belong to same term symbol, having different seniority number. Gram-Schmidt procedure was used to make them orthogonal.
International Reviews in Physical Chemistry, 2010
In this review, we address computation of diatomic molecular spectra. An overview of the theory is discussed based on symmetries of the diatomic molecule. The standard quantum theory of angular momentum fully accounts for the rotational states of the diatomic molecule. Details are elaborated in view of standard versus anomalous commutators for generation of a synthetic spectrum. Specific example spectra are presented for selected diatomic molecules in view of diagnostic applications in laser-induced optical breakdown spectroscopy.
Journal of Molecular Structure, 2010
The experimental rotational spectrum of 5-oxo-1,3,2,4-dithiadiazole (Roesky's ketone) has been recorded and the experimental rotational constants have been determined. The latter have been used to evaluate the performance of a large number of quantum chemical methods combined with different basis sets, by comparing the calculated with the experimental values. The results of this comparison indicate that, in general, the wave-function-based methods perform better than those from Density Functional Theory. Four of the 42 investigated method/basis set combinations prove to be the most valuable, i.e., MP4(SDQ)/(aug-)cc-pVTZ, B3PW91/cc-pV(T+d)Z and MPW1PW91/aug-cc-pVTZ, as they produce rotational constants with a root-mean-square deviation from the experimental values of only about 5 MHz. j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / m o l s t r u c sets, based on the root-mean-square (rms) difference between the experimental and calculated values.
International Journal of Quantum Chemistry, 2011
Starting with the Hamilton-Jacobi equation, Campos et al. have applied Hylleraas' method along with the series obtained by Wind-Jaffe to several molecular ions, among which the H + 2 system, to determine their electronic energies in different states. In this work, we have fitted the potential energy curves for the 2pπ, 3dσ , 4dσ , 4f π, 4f σ , 5gσ , and 6iσ electronic states of the H + 2 ion employing the Rydberg generalized function. From these fittings, the spectroscopic constants and the rovibrational energies have been determined by two distinct methods: Dunham's and the discrete variable representation. The theoretically obtained results are in a satisfactory agreement and are expected to provide a comparison source to future works in the experimental field.
A method for using a single Kindependent grid for problems where otherwise a basis of associated Legendre functions or the corresponding K-dependent grids would be employed, specific&y for calculating the rotational-vibrational energy Ievels of a triatomic molecule, has been described and tested. K independence has been achieved by the incorporation of the weight functions of associated Legendre functions into the Hamiltonian. Exact analytical expressions, valid for any DVR basis, of the matrix elements of the ro~tion-bending kinetic energy operator (in terms of scattering coordinates f have been given. Simple numerical tests demonstrate that this new method is a useful ahemative to the methods proposed so far.
Quantum Mechanical Electronic Structure Calculations with Chemical Accuracy, 1995
In the first section of this thesis, we present the atomic part of our investigation.
The Journal of Chemical Physics, 1986
The Journal of Chemical Physics, 1965
The Journal of Chemical Physics, 2007
Rovibrational spectra of Ar 3 are computed for total angular momenta up to J = 6 using row-orthonormal hyperspherical coordinates and an expansion of the wave function on hyperspherical harmonics. The sensitivity of the spectra to the two-body potential and to the three-body corrections is analyzed. First, the best available semiempirical pair potential ͑HFDID1͒ is compared with our recent ab initio two-body potential. The ab initio vibrational energies are typically 1-2 cm −1 higher than the semiempirical ones, which is related to the slightly larger dissociation energy of the semiempirical potential. Then, the Axilrod-Teller asymptotic expansion of the three-body correction is compared with our newly developed ab initio three-body potential. The difference is found smaller than 0.3 cm −1 . In addition, we define approximate quantum numbers to describe the vibration and rotation of the system. The vibration is represented by a hyper-radial mode and a two-degree-of-freedom hyperangular mode, including a vibrational angular momentum defined in an Eckart frame. The rotation is described by the total angular momentum quantum number, its projection on the axis perpendicular to the molecular plane, and a hyperangular internal momentum quantum number, related to the vibrational angular momentum by a transformation between Eckart and principal-axes-of-inertia frames. These quantum numbers provide a qualitative understanding of the spectra and, in particular, of the impact of the nuclear permutational symmetry of the system ͑bosonic with zero nuclear spin͒. Rotational constants are extracted from the spectra and are shown to be accurate only for the ground hyperangular mode. Downloaded 04 May 2007 to 130.120.230.129. Redistribution subject to AIP license or copyright, see http://jcp.aip.org/jcp/copyright.jsp M J d D ͑⍀͒.
Symmetries in Science X, 1998
We discuss a symmetry-adapted algebraic (or vibron) model for molecular spectroscopy. The model is formulated in terms of tensor operators under the molecular point group. In this way, we have identified interactions that are absent in previous versions of the vibron model, in which the Hamiltonian is expressed in terms of Casimir operators and their products. The inclusion of these new interactions leads to reliable spectroscopic predictions. As an example we study the vibrational excitations of the methane molecule, and compare our results with those obtained in other algebraic models.
Journal of Mathematical Chemistry, 2015
Spectroscopic techniques are very essential tools in studying electronic structures, spectroscopic constants and energetic properties of diatomic molecules. These techniques are also required for parametrization of new method based on theoretical analysis and computational calculations. In this research, we apply the proper quantization rule in spectroscopic study of some diatomic molecules by solving the Schrödinger equation with two solvable quantum molecular systems-Tietz-Wei and shifted Deng-Fan potential models for their approximate nonrelativistic energy states via an appropriate approximation to the centrifugal term. We show that the energy levels can be determined from its ground state energy. The beauty and simplicity of the method applied in this study is that, it can be applied to any exactly as well as approximately solvable models. The validity and accuracy of the method is tested with previous techniques via numerical computation for H 2 and CO diatomic molecules. The result also include energy spectrum of 5 different electronic states of NO and 2 different electronic state of ICl.
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