Molecular-level Design of Heterogeneous Chiral Catalysts

It has been shown previously that the adsorption of a chiral 2-butanol template on Pd(111) leads to enantioselective adsorption of chiral propylene oxide probe molecules. Enantioselectivity is expressed over a narrow coverage range where the maximum value of enantioselectivity ratio (ER defined as Θ(R-propylene oxide)/Θ(S-propylene oxide), where Θ is the coverage) reaches ~2. Probe coverages in this case were measured using either reflection-absorption infrared spectroscopy (RAIRS) or temperature-programmed desorption (TPD) [1,2]. The enantioselectivity disappears when the 2-butanol-covered surface was heated to ~200 K since the adsorbed butoxy species decomposes by a β-hydride elimination reaction to yield a non-chiral ketone. Monte Carlo calculations of the effect of chiral modifiers have yielded results that are consistent with these experimental observations [3,4]. Similar experiments using 2-methyl butanoic acid as a template, where the chiral center is identical to that in 2-butanol but is now anchored by a carboxylate group rather than by an alkoxide, shows no enantioselectivity. In this case, propylene oxide coverages were measured using the King and Wells method. RAIRS experiments and density functional calculations suggest that the 2-butyl group of the 2-butoxy species is oriented parallel to the surface. A possible origin for the lack of enantioselectivity of a 2-methyl more » butanoic acid-covered surface may be that the 2-butyl group is farther from the surface, allowing it to rotate more freely, averaging out any asymmetry, resulting in a loss of chirality. In order to test this idea, the alkyl group on the carboxylic acid was functionalized with an amine to anchor the chiral center to the surface. Using the amino-acids alanine and 2-amino butanoic acid as templates restored the enantioselectivity and yielded ER values of 2.0 ± 0.2 and 1.75 ± 0.15 respectively. These results suggest that a two-point attachment of the chiral template is required, one for surface adsorption and the other to allow the enantioselectivity to be expressed. Low-energy electron diffraction (LEED) intensity versus energy (I/E) measurements are used to measure the structure of templates and probes on the Pd(111) surface, where these results will be compared with calculations carried out by the Sholl group. Since the aminoacids are relatively large, initial experiments were carried out to determine the structure of carboxylates on the surface to determine the carboxylate group anchoring site. Since carboxylates do not form ordered structures on Pd(111), we have exploited a method recently developed in collaboration with Professor Saldin to measure structures of disordered overlayers [5]. Results show that the formate OCO plane is oriented perpendicular to the surface with the oxygen atoms located across a short bridge on the (111) surface. The effect of the size of the functional group on the amino acid template (RCH(NH2)COOH) was also investigated where the maximum ER values obtained using propylene oxide were 2.0 ± 0.2 (R=CH3), 1.75 ± 0.15 (R=C2H5), 1.65 ± 0.15 (R=C3H6) and 1.30 ± 0.15 (R=CH2CH(CH3)2) thus showing a decreasing trend with increasing size of the side chain. The enantioselectivity of S-(1-naphthyl) ethylamine-covered surfaces have been explored using propylene oxide as a probe, but these systems showed no enantioselectivity. However, using 2-butanol as a probe lead to enantioselective chemisorption implying that one-to-one modification requires a direct hydrogen-bonding interaction between the probe and modifier. 1. Enantioselective Chemisorption on a Chirally Patterned Surface in Ultrahigh Vacuum: Adsorption of Propylene Oxide on 2-butoxy-Covered Pd(111), D. Stacchiola, L. Burkholder and W.T. Tysoe, J. Am. Chem. Soc., 124, 8984 (2002) 2. Enantioselective Chemisorption on a Chirally Modified Surface in Ultrahigh Vacuum: Adsorption of Propylene Oxide on 2-butoxide-Covered Pd(111), Dario Stacchiola, Luke Burkholder and Wilfred T. Tysoe, J. Mol. Catal A: Chemical, 216, 215 (2004) 3. Theoretical Analysis of the Coverage Dependence of Enantioselective Chemisorption on a Chirally Patterned Surface, F. Roma, D. Stacchiola, G. Zgrablich and W. T. Tysoe, Journal of Chemical Physics, 118, 6030 (2003) 4. Lattice-gas Modeling of Enantioselective Adsorption by Template Chiral Substrates, F. Roma, D. Stacchiola, W.T. Tysoe and G. Zgrablich, Physica A., 338, 493 (2004) 5. Structure Determination of Disordered Organic Molecules on Surfaces from the Bragg Spots of Low Energy Electron Diffraction and Total Energy Calculations, H. C. Poon, M. Weinert, D. K. Saldin, D. Stacchiola, T. Zheng and W. T. Tysoe, Phys. Rev. B., 69, 35401 (2004) « less