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PREFACE The Thesis entitled "Spectroscopic properties of diatomic molecules ' deals with the results of the electronic spectra of the diatomic molecules H2. NdO, CaO, SiO, SiO+, FeH, N2+, VO, CaF and BaF. The thesis is divided into five chapters and a brief summary of each chapter is as follows: Chapter 1 describes the spectroscopic properties of diatomic molecules which are useful in the fields of astrophysics, gas kinetics, chemical physics etc. Some of the applications are as follows: The abundance (concentration) of molecular species can be estimated from the intensities of interstellar lines. The temperature of interstellar atmosphere can be determined by band-spectroscopic methods. And, the study of interstellar band spectra specifically gives information about abundance ratio of isotopes. The spectroscopic data allows to predict reliable values of heat capacities even for chemically unstable diatomic gases for which direct thermal measurements are impossible. In addition to heat content and heat capacity, the entropy and free energy of a gas can be calculated once the partition function has been obtained from the spectroscopic data. Also, the equilibria of chemical reactions in gases can be predicted on the basis of spectroscopic data. The nuclear properties such as nuclear magnetic moment, nuclear quadruple moment etc., can be determined from the investigations of molecular spectra. The heats of the elementary chemical reactions, which are not accessible to direct measurement, can be calculated accurately from the dissociation energies of the molecules involved. Molecular spectra provide the most useful data for determining molecular structures and bond energies, and are a key means of verifying the presence of various elements or molecules and monitoring the concentrations of chemical species in laboratory, industrial, atmospheric and interstellar environments. Frank-Condon factors are important parameters for every molecular band system, since they enter into the calculation of the relative band intensity, which is a significant source of information in quantitative spectroscopy, high-temperature chemistry, astrochemistry and cometary spectra. They are also important for the determination of the molecular structure, population of the vibrational levels in the upper electronic state involved in a transition, radiative lifetime, vibrational temperature and kinetics of energy transfer in stellar and other astrophysical atmospheres containing molecular species. On the other hand, knowledge of rCentroids has been found to be very useful in the discussion of the variation of the electronic transition moment with internuclear separation and in other molecular properties. Variation of r-Centroids with band wavelengths (or wavenumbers) provides a useful bridge between experimental measurements, which are often expressed as a function of wavelength and theoretical studies, which are often made in terms of internuclear separation. The electronic and vibrational energy levels of a diatomic molecule in a given electronic state are often described by a potential energy (Y-axis) internuclear distance (X-axis) diagram. Each electronic state of a molecule is a characteristic of its own potential energy curve. Consequently, the collection of a number of such potential energy curves, presents an equivalent representation of the corresponding electronic states of the molecules. The potential energy curve for any electronic state of a diatomic molecule can be represented by an empirical potential function. Morse function is one of the most successful empirical potential functions among a number of simple and approximately good empirical analytical functions. However in many cases, the assembly of energy levels cannot be an exact representative model of the molecule over a wide experimental range of energies. In order to overcome this problem and to obtain appropriate potential energy curves from the band spectroscopic data Vanderslice et al, developed a modified method known as Rydberg-Klein-ReesVanderslice (RKRV) method. n Chapter 2 describes the details of the RKRV method for the construction of potential energy curves of certain diatomic molecules. The construction of experimental potential energy curves for the selective 26 electronic states of 10 specified diatomic molecules dealt in this chapter and, listed below: S.No. Molecule Electronic states 1 h2 X 'l+g, B 'X+u and C 'flu 2 NdO X( 1)4, (1)3 and [10.935]4 3 CaO X , A 'l+ and a 3flo- 4 SiO X r and E T 5 SiO+ X 2I, A 6 FeH X4A and F 4A 7 NT X 2X~. A 2n{1 and B2X~ 8 VO X4X k and 2[]i 9 CaF X 2IT A 2n and B 2X+ 10 BaF X 2I^ and A 2n 2n and B 2X+ 2 In accordance with the report of Wilkinson the information of dissociation energies and ionization potentials of diatomic molecules is helpful to decipher many astrophysical, as well as physical and chemical problems. Chapter 3 emphasis the details of several methods exist in the literature for the determination of the bond energies. Nevertheless, the determination of dissociation energy is also carried out by the spectroscopic method based on pre-dissociation limit. In the case of diatomic molecules, the pre- dissociation limit yields only the upper limit of the dissociation energy. As per Henri, this phenomenon in which the bands corresponding to transitions to low vibrational levels of the upper electronic state exhibit a normal type of rotational structure consists of various sharp lines. But. iii the transition to higher vibrational levels gives bands in which the lines of the rotational fine structure are relatively diffused. The reason of this diffuseness as attributed to some instability in the molecules is also discussed. As any of the experimental potential energy curves are insufficient by themselves for the estimation of dissociation energy of a molecule, a relevant analytical expression developed is felt very much needed owing of their greater influence. In the present work, Hulburt-Hirschfelder function, is chosen to estimate dissociation energies of H2, NdO, CaO, SiO, SiO+, FeH, N2+, VO, CaF and BaF. Chapter 4 gives the importance of the internuclear distance in describing the structure and properties of diatomic molecules. When a molecule absorbs visible or ultraviolet light, a new excited state with modified electronic structure replaces the original electronic structure. This occurs on such a short time scale that there is no significant change in the internuclear distance (i.e., in the position of the nuclei) of the molecule. Such a change i.e., the transition between the two states is described as vertical. An overview of the vibrational wave functions pertaining to the ground and excited states are revealing that the overlap of these wave functions will determine the intensity of the transition. After an electronic transition, the excited state immediately restores back to its equilibrium bond length. The concept of a vertical transition i.e.. at constant internuclear distance stands as the central point for the discussion of the Franck-Condon principle. The concept of r-Centroids was introduced by Fraser, Nicholls and Jarmain during their study of the variation of molecular parameters with internuclear separation. It is defined as the r-coordinate of the Centroids of the area represented by the overlap integral and takes a unique value for each band of a transition system. IV In the present work, the r-Centroids are determined using quadratic equation method of Nicholls and Jarmain for the following 7 transitions in the case of 7 diatomic molecules. They are: Transitions S.No. Molecule 1 h2 2 CaO a3no. - X 3 VO 1U2- x4 rk 4 n2+ A2riu, 5 SiO+ A2n-* x2r 6 SiO E 'S+-^ Xf+ 7 BaF A 2if -+ X2I+ B'ru- - vlv+ A i-* a x4eu" The trends of r-Centroids for the characteristics transitions are discussed in detail, in the wake of the qualitative importance of atoms that constitute the molecule under study. The dependence of relative intensity (of vibrational bands in spectra) on the square of the vibrational overlap integrals (of the electronic states) which are involved in the transitions is discussed in this Chapter. These transitions are usually known as the vibrational transition probabilities (Franck-Condon factors). Chapter 5 highlights the importance of Franck-Condon factors and their wide applicability in many branches of physics and chemistry. In the spirit of Franck's mathematical idea and as later developed (on wave mechanical basis) by Condon, a possible explanation for the intensity distribution in the energy level band system of a diatomic molecule, is also explained. As such, the resulting Franck-Condon factor arrays happen to be the basic molecular data needed in the interpretation of intensities of molecular spectra. The important role of Franck-Condon factors for the calculation of vibrational transition probabilities of diatomic molecules is presented. A vivid literature survey with details of different methods employed to evaluate the Franck-Condon factors, is also presented. In the present work, the Franck-Condon factors are evaluated by the specific approximate analytical method of Fraser and Jarmain. The Franck-Condon factors are determined for the following 15 systems belonging to 10 different diatomic molecules during the specified transitions. S.No, Molecule 1 h2 2 NdO 3 CaO 4 FeH 5 VO 6 NT 7 SiO+ X ’x+„ (1)3 - X(l)4, AX+X, F4A- x4a 1 2Um ■ X A2nul X 4XU+ A2n- x 2r, 8 SiO E 'Xf- 9 CaF A2n- x 2r, 10 BaF A2nr- A comparative Transitions B 'X+u and cnu-- X 'x+ [10.935]4 -■* X 'x+ a Jn» -->x b 2r-> x 2r xr b 2r-^ x 2r X2X+ systematic study of Franck-Condon factors corresponding to different transitions is described as a function of characteristic properties of the constituent atoms of the molecule. VI Major portion of the work presented in the thesis has been published by the author in the following scientific journals. 1. Spectroscopic Studies of Astrophysical important molecules. Astrophysics and Space Science (Submitted for publication) . 22.Dissociation Energies of VO, FeH, BaF and NdO Molecules. Indian Journal of pure and Applied Physics. (In Press). 3. Estimation of Potential Energy curves, Dissociation Energies, Condon Factors and r-Centroids of Fl2. CaF and SiO+ Molecules. (Submitted to JQSRT). Vll Franck-