Microwave rotational spectrum and ab initio equilibrium structure of fumaric acid: Anharmonicity bridging the molecular characterizations
Graphical abstract
Accurate rotational constants of fumaric acid are obtained by supersonic-jet Fourier transform microwave spectroscopy. Comparison with high-level ab initio structure calculations, requires anharmonicity effects in the vibrational ground-state to be calculated.
Highlights
► Fumaric Acid is observed by supersonic jet expansion microwave spectroscopy. ► Spectroscopic constants and electric dipole moments are obtained at high accuracy. ► Spectroscopic and ab initio data agree on a low-energy s-cis,s-trans conformer. ► Experiment and theory are compatible when anharmonic effects are taken into account.
Introduction
Fumaric and maleic acid, being the trans and cis isomers of butenedioic acid, respectively, are the simplest dicarboxylic acids with a CC double bond. Besides being a prototype dicarboxylic acid, fumaric acid is of practical interest due to its applications in medicine (e.g. as anti-tumoral agent, an inhibitor of transaminase reactions) and in polymer chemistry [1], [2]. The accurate determination of its molecular constants is important for a fundamental understanding of its chemical properties.
Previously, the molecular structure of fumaric acid was studied twice by gas-phase electron diffraction (GED). In the earlier study at 533 K [3], the structural analysis was carried out, assuming a single conformer with both CO bonds in antiperiplanar (ap) positions relative to the CC bond (s-trans arrangements, see conformer III in Fig. 1). However, the recent GED reanalysis [4] has shown that, in the gas-phase at 480 K, fumaric acid constitutes a mixture of three conformers in approximately equal amounts. These conformers exhibit either two s-cis (I), or two s-trans (III), or one s-cis and one s-trans (II) OCCC arrangements (see Fig. 1). The same conformational composition of fumaric acid was revealed in the analysis of infrared (IR) vibrational spectra observed in an Ar matrix and assigned with use of scaled harmonic frequencies from the B3LYP/6-31G(d,p) calculations [5]. Recent MP2/cc-pVTZ calculations [4], predict six stable conformations for fumaric acid. The low-energy conformers have both OCOH fragments in synperiplanar (sp) positions, while the high-energy conformers have one or two OCOH groups in ap positions. The relative energies of the three low-energy conformers I–III were calculated to be 0 kJ mol−1, 1.5 kJ mol−1 and 2.7 kJ mol−1 (MP2/cc-pVQZ), respectively [4]. According to this ab initio prediction, the conformers exist in a ratio of I:II:III = 33:48:19 at 480 K, whereas the high-energy conformers are practically absent at this temperature. Since the conformers I and III, both belonging to the point group C2h, have no permanent dipole moments, only the most abundant conformer II (point group Cs) exhibits a rotational spectrum and can thus be detected by microwave (MW) spectroscopy.
The aim of the present work is a high-resolution study of the vibrational ground-state rotational spectra of fumaric acid by supersonic jet expansion Fourier-transform (FT) MW spectroscopy while employing high-level ab initio calculations to deduce semi-experimental equilibrium constants.
Section snippets
Experimental
As no microwave study on fumaric acid has been reported earlier, spectral surveys for the rotational spectrum of this molecule were done using a high resolution Fourier-transform microwave (FT-MW) spectrometer – a pulsed supersonic jet-expansion Fabry–Pérot-type resonator spectrometer of the Balle–Flygare design [6], [7]. The sample of fumaric acid (Aldrich, 99%) was used without further purification. Fumaric acid is a white solid at room temperature; it melts at 287 °C. To obtain sufficient
Quantum-chemical calculations
The geometries of low-energy conformers I–III were optimized at the coupled cluster CCSD(T) level of theory [15], [16] with the correlation-consistent polarized valence triple zeta (cc-pVTZ) basis set [17]. The coupled cluster T1 diagnostic [18] was also calculated in the CCSD(T)/cc-pVTZ approximation. As it has been shown in Refs. [19], [20], [21], the small changes in the geometrical parameters due to the improvement of the basis set and the electron correlation approximation at the CCSD(T)
Discussion and conclusions
As it can be seen from Table 6, the higher the level of ab initio calculations, the closer the computed structural parameters approach the semi-experimental equilibrium geometry determined from the GED data supplemented by the ab initio cubic force field [4]. The bond lengths in the MP2/cc-pVTZ approximation are longer than the GED values by up to 0.008 Å, while the differences between the MP2/cc-pV5Z (or MP2/cc-pVQZ) and GED values are outside of experimental uncertainties only by about 0.001 Å.
Acknowledgments
We gratefully acknowledge support from the Deutsche Forschungsgemeinschaft (DFG), the Land Niedersachsen, and the Dr. Barbara Mez-Starck Foundation, and especially the assistance of J. Demaison in the treatment of anharmonic effects.
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