Co-reporter:Kyle J. Mascaritolo, Ivan O. Antonov, Michael C. Heaven
Journal of Molecular Spectroscopy 2014 Volume 297() pp:1-3
Publication Date(Web):March 2014
DOI:10.1016/j.jms.2014.01.004
•The 2Π(4p) state of the AlAr van der Waals complex has been observed using two-photon excitation.•2Π(4p) zero-point spin–orbit coupling constant was found to be 18.5 cm−1.•Potential curve fitting yielded an equilibrium distance of 3.33 Å and a well depth of De = 495 cm−1.The 2Π(4p)–X2Π(3p) band system of AlAr has been observed using two-photon excitation. The spectrum consists of a short progression of doublet bands, with spin–orbit intervals that are close to that of Al(4p). Potential energy curve fitting yielded a bond dissociation energy for 2Π(4p) of De = 495(5) cm−1 and an approximate bond length of Re = 3.33(4) Å.Graphical abstract
Co-reporter:Michael C. Heaven, Vladimir E. Bondybey, Jeremy M. Merritt, Alexey L. Kaledin
Chemical Physics Letters 2011 Volume 506(1–3) pp:1-14
Publication Date(Web):11 April 2011
DOI:10.1016/j.cplett.2011.02.025
Abstract
Having closed valence sub-shells, the alkaline earth atoms participate in covalent bonding via orbital hybridization and exchange interactions, with additional contributions from dispersion interactions. Starting from a closed ns2 configuration imparts different characteristics to the chemistry of this group, as compared to metals that have open-shell atomic ground states. Theoretical studies of the bonding of the Group IIA metals have been pursued for many years, and they are known to be challenging for ab initio electronic structure methods. The bonding motifs have been examined, and the differences between beryllium and the remainder of the group explored. Experimental studies that probe the bonding, particularly for beryllium, have lagged behind the theoretical work. In the present Letter we describe our recent spectroscopic and theoretical investigations of simple beryllium compounds, and discuss these results in terms of their relationship to the properties of the heavier Group IIA elements.
Co-reporter:K. Freel, J. Park, M.C. Lin, Michael C. Heaven
Chemical Physics Letters 2011 Volume 507(4–6) pp:216-220
Publication Date(Web):9 May 2011
DOI:10.1016/j.cplett.2011.03.081
Co-reporter:Jeremy M. Merritt, Alexey L. Kaledin, Vladimir E. Bondybey and Michael C. Heaven
Physical Chemistry Chemical Physics 2008 vol. 10(Issue 27) pp:4006-4013
Publication Date(Web):29 May 2008
DOI:10.1039/B803975E
Low lying electronic states of the beryllium dimer were investigated by laser induced fluorescence (LIF) and resonance enhanced multiphoton ionization (REMPI) techniques. Be2 was formed by pulsed laser ablation of Be metal in the presence of helium carrier gas, followed by a free jet expansion into vacuum. Several previously unobserved states of the dimer were characterized. These included transitions of the triplet manifold (2)3Πg ← (1)3Σ+u and (3)3Πg ← (1)3Σ+u, for which rotationally resolved bands were obtained. In addition, transitions to the v′ = 10–18 vibrational levels of the A1Πu state were recorded. Photoionization efficiency (PIE) measurements were used to determine an accurate ionization energy (IE) for Be2 of 7.418(5) eV and the term energy for (1)3Σ+u. Above the ionization threshold the PIE spectrum was found to be highly structured, consisting of overlapping Rydberg series that converged on excited vibrational levels of Be2+. Analysis of these series yielded a vibration frequency for the X2Σ+u state of 498(20) cm−1. The bond dissociation energy for Be2+, deduced from the IE measurement, was 16072(40) cm−1. Multi-reference configuration interaction (MRCI) calculations were carried out for Be2 and Be2+, yielding results that were in excellent agreement with the experimental observations.
Co-reporter:Galina Kerenskaya, Udo Schnupf, Michael C. Heaven, Ad van der Avoird and Gerrit C. Groenenboom
Physical Chemistry Chemical Physics 2005 vol. 7(Issue 5) pp:846-854
Publication Date(Web):06 Jan 2005
DOI:10.1039/B415253K
A study of NH/D–Ne was undertaken to investigate the structure of this complex and examine the ability of high-level theoretical methods to predict its properties. The A 3Π–X 3Σ− transition was characterized using laser induced fluorescence measurements. Results from theoretical calculations were used to guide the interpretation of the spectra. Two-dimensional potential energy surfaces were calculated using second-order multireference perturbation theory with large correlation consistent basis sets. The potential energy surfaces were used to predict the ro-vibronic structure of the A–X system. Calculated ro-vibronic energy level patterns could be recognized in the spectra but quantitative discrepancies were found. These discrepancies are attributed to incomplete recovery of the dynamical correlation energy.
Co-reporter:Michael C Heaven, Alexei A Buchachenko
Journal of Molecular Spectroscopy 2003 Volume 222(Issue 1) pp:31-45
Publication Date(Web):November 2003
DOI:10.1016/S0022-2852(02)00057-7
The effects of relative orientation on collision and reaction dynamics can be examined by characterizing the unimolecular decay of van der Waals complexes. Most commonly, decomposition is initiated by exciting one of the monomers within a complex, and the relative orientation is defined by the zero-point motions for the intermolecular degrees of freedom. However, if simultaneous excitation of the intermolecular degrees of freedom is achieved, a considerable range of starting configurations may be accessed. We are currently studying I2–Rg and CN–H2/D2 complexes with the goal of using these systems to examine oriented dynamics. For I2(B)–Ne we have observed excited intermolecular vibrations and the effects of these motions on the predissociation dynamics. The correlation between structure and dynamics suggested by these results can be understood using classical mechanics, but the implications of this model are at variance with accepted ideas about the topology of I2(B)–Rg potential surfaces. Spectroscopic and theoretical studies of CN–H2/D2 indicate that this pre-reactive complex may be used to examine steric effects in the H2+CN→H+HCN reaction. The complex was characterized using the A–X and B–X electronic transitions. As is often the case for weakly bound systems, the insights provided by high-level theoretical calculations were essential for interpretation of the spectra. The properties of excited intermolecular vibrations of CN–H2 were predicted as a prelude to studies of the intra-cluster reaction dynamics.
Co-reporter:Jeremy M. Merritt, Alexey L. Kaledin, Vladimir E. Bondybey and Michael C. Heaven
Physical Chemistry Chemical Physics 2008 - vol. 10(Issue 27) pp:NaN4013-4013
Publication Date(Web):2008/05/29
DOI:10.1039/B803975E
Low lying electronic states of the beryllium dimer were investigated by laser induced fluorescence (LIF) and resonance enhanced multiphoton ionization (REMPI) techniques. Be2 was formed by pulsed laser ablation of Be metal in the presence of helium carrier gas, followed by a free jet expansion into vacuum. Several previously unobserved states of the dimer were characterized. These included transitions of the triplet manifold (2)3Πg ← (1)3Σ+u and (3)3Πg ← (1)3Σ+u, for which rotationally resolved bands were obtained. In addition, transitions to the v′ = 10–18 vibrational levels of the A1Πu state were recorded. Photoionization efficiency (PIE) measurements were used to determine an accurate ionization energy (IE) for Be2 of 7.418(5) eV and the term energy for (1)3Σ+u. Above the ionization threshold the PIE spectrum was found to be highly structured, consisting of overlapping Rydberg series that converged on excited vibrational levels of Be2+. Analysis of these series yielded a vibration frequency for the X2Σ+u state of 498(20) cm−1. The bond dissociation energy for Be2+, deduced from the IE measurement, was 16072(40) cm−1. Multi-reference configuration interaction (MRCI) calculations were carried out for Be2 and Be2+, yielding results that were in excellent agreement with the experimental observations.