We have calculated the vibrational solvent shifts of the fundamental bands of HCl diluted in Ar, Kr, and Xe solutions at different thermodynamic conditions by means of the molecular dynamics technique and a model for the isotropic part of the interaction depending on the vibration. The theoretical vibrational shifts, which were compared with the available experimental data, have been determined by considering both, the usual linear Buckingham terms and the nonlinear anharmonic corrections, and the latter omitted in a previous work for the HCl in Ar and Kr. We have found that the Buckingham contributions dominate the solvent shifts of the fundamental bands of HCl in Ar, Kr, and Xe, although the anharmonic shifts’ present significant greater values than those obtained previously for N2 diluted in liquid Ar and pure liquid N2, both at normal conditions. We have analyzed the solvent shifts influence of the linear and quadratic (in the vibrational coordinate) oscillator-bath interaction terms and also the Dunham intramolecular potential effects on the anharmonic contributions. 1. Introduction The study of the fundamental and overtones infrared and Raman vibrational solvent shifts gives relevant information about the molecular interaction depending of the intramolecular vibration [1–7]. In an earlier work, according to Buckingham, it was deduced that the diatomic solvent shift associated to the vibrational transition of a cubic anharmonic oscillator presents a linear dependence with the vibrational quantum number [1]. This result, which is valid in principle for the fundamental band or lower overtones of several diatomics, would break down for the fundamental bands of some molecules and high overtones of much ones. Recently, Alessi et al. [6, 7] has deduced the non-linear ( ) correction (anharmonic correction) to the linear Buckingham solvent shift for a diatomic molecule perturbed by an atomic or molecular solvent. Alessi et al. [6, 7] analyzed the solvent shift of N2 diluted in liquid Ar and pure N2 liquid, both at normal conditions, founding that the non-linear solvent correction, also called anharmonic shift [6, 7], represents only the 1% of the fundamental shift of the isotropic Raman band. This result is due in part to the small anharmonicity parameter of N2 ( ) [6, 7]; however, because the HCl anharmonicity constant is clearly much larger than the N2 one, we expect a major contribution of non-linear solvent shift for the fundamental band of HCl diluted in Ar, Kr, and Xe. We have made a previous study [8] of the vibrational solvent shifts of HCl diluted
References
[1]
A. D. Buckingham, “Solvent effects in vibrational spectroscopy,” Transactions of the Faraday Society, vol. 56, pp. 753–760, 1960.
[2]
D. W. Oxtoby, “Dephasing of molecular vibrations in liquids,” Advances in Chemical Physics, vol. 40, 1979.
[3]
D. W. Oxtoby, “Vibrational relaxation in liquids,” Annual Review of Physical Chemistry, vol. 32, pp. 77–101, 1981.
[4]
J. P. J. Michels, M. I. M. Scheerboom, and J. A. Schouten, “Computer simulations of the linewidth of the Raman Q-branch in fluid nitrogen,” Journal of Chemical Physics, vol. 103, no. 19, pp. 8338–8345, 1995.
[5]
K. F. Everitt and J. L. Skinner, “Isotropic Raman line shapes of N2 and O2 along their liquid-gas coexistence lines,” Journal of Chemical Physics, vol. 115, no. 18, pp. 8531–8539, 2001.
[6]
N. Alessi, I. S. Tolokh, S. Goldman, and C. G. Gray, “Simulation study of solvent shifts of vibrational overtone spectra,” Molecular Physics, vol. 102, no. 19-20, pp. 2037–2047, 2004.
[7]
N. Alessi, I. S. Tolokh, S. Goldman, and C. G. Gray, “Simulation study of N2 overtone solvent shifts using improved potentials,” Molecular Physics, vol. 103, no. 17, pp. 2381–2396, 2005.
[8]
A. Padilla and J. Pérez, “The fundamental vibrational shift of HCl diluted in dense Ar and Kr,” Molecular Physics, vol. 106, no. 5, pp. 687–691, 2008.
[9]
P. Marteau, C. Boulet, and D. Robert, “Finite duration of collisions and vibrational dephasing effects on the Ar broadened HF infrared line shapes: asymmetric profiles,” Journal of Chemical Physics, vol. 80, no. 8, pp. 3632–3639, 1984.
[10]
S. L. Holmgren, M. Waldman, and W. Klemperer, “Internal dynamics of van der Waals complexes. II. Determination of a potential energy surface for ArHCl,” Journal of Chemical Physics, vol. 69, no. 4, pp. 1661–1669, 1978.
[11]
J. M. Hutson and B. J. Howard, “Anisotropic intermolecular forces,” Molecular Physics, vol. 45, no. 4, pp. 769–790, 1982.
[12]
J. Pérez, A. Padilla, W. A. Herrebout, B. J. Van Der Veken, A. C. Hernández, and M. O. Bulanin, “Experimental analysis and modified rotor description of the infrared fundamental band of HCl in Ar, Kr, and Xe solutions,” Journal of Chemical Physics, vol. 122, no. 19, Article ID 194507, 9 pages, 2005.
[13]
A. Padilla, J. Pérez, and A. Calvo Hernández, “Vibrorotational Raman and infrared spectra of polar diatomic molecules in inert solutions. I. Spectral theory,” Journal of Chemical Physics, vol. 111, no. 24, pp. 11015–11025, 1999.
[14]
C. G. Gray and K. E. Gubbins, Theory of Molecular Fluids, vol. I, Claredon Press, Oxford, UK, 1984.
[15]
L. Bonamy and P. N. M. Hoang, “Far infrared absorption of diatomic polar molecules in simple liquids and statistical properties of the interactions. I. Spectral theory,” Journal of Chemical Physics, vol. 67, pp. 4423–4430, 1977.
[16]
A. Medina, J. M. M. Roco, A. C. Hernández et al., “Vibration-rotation spectra of HCI in rare-gas liquid mixtures: molecular dynamics simulations of Q-branch absorption,” Journal of Chemical Physics, vol. 116, no. 12, pp. 5058–5065, 2002.
[17]
M. O. Bulanin and K. G. Tokhadze, Optics and Spectroscopy, vol. 61, p. 198, 1986.
[18]
V. V. Bertsev and G. Ya. Zelikina, “Electronic absorption spectra of some cryosystems,” in Molecular Cryospectroscopy, R. J. H. Clark and R. E. Hester, Eds., John Wiley & Sons, Chichester, UK, 1995.
[19]
D. P. Tassios, Applied Chemical Engineering Thermodynamics, Springer, Berlin, Germany, 1993.
[20]
G. Guelachvili, P. Niay, and P. Bernage, “Infrared bands of HCl and DCl by Fourier transform spectroscopy. Dunham coefficients for HCl, DCl, and TCl,” Journal of Molecular Spectroscopy, vol. 85, no. 2, pp. 271–281, 1981.
[21]
M. O. Bulanin, K. Kerl, A. Padilla, J. Pérez, and A. Calvo Hernández, “First vibrational overtone bandshape of HCl in fluid SF6: an experimental and theoretical study,” Physical Chemistry Chemical Physics, vol. 2, pp. 5375–5382, 2000.