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Updated: Jan 24, 2026

Characterizing Lewis Pairs Using Titration Coupled with In Situ Infrared Spectroscopy
Published on: February 20, 2020
Dihydrogen Splitting by Intramolecular Borane-Phosphane Frustrated Lewis Pairs: A Comprehensive Characterization
Robert Knitsch1, Thomas Özgün2, Guo-Qiang Chen2
1Institut für Physikalische Chemie, WWU Münster, Corrensstraße 30, D-41849, Münster, Germany.
Abstract:
Four hydrogenated intramolecular phosphane-borane frustrated Lewis pair (B/P FLP) compounds bearing unsaturated cyclic or aromatic carbon backbones have been synthesized and structurally characterized using 11 B, 31 P, 1 H and 2 H solid-state NMR spectroscopy. A comparison of the spectra with those of the corresponding free B/P FLPs shows that both 11 B isotropic chemical shifts as well as nuclear electric quadrupolar coupling constants decrease significantly upon FLP hydrogenation, revealing the breakage of the partial B-P bond present in the starting materials. Likewise, the 31 P isotropic chemical shift, the chemical shift anisotropy, and the asymmetry parameter decrease significantly upon FLP hydrogenation, reflecting the formation of a more symmetric, C3v -like local environment. 11 B{31 P} rotational echo double resonance (REDOR) experiments can be used to measure the B-P internuclear distance (about 3.2 Å) of these compounds. Observation of the hydrogen atoms bound to the Lewis centers is best accomplished via 31 P{1 H} and 11 B{1 H} cross-polarization-heteronuclear correlation experiments or by direct observation of the 2 H MAS NMR signals on especially prepared FLP-D2 adducts. For accurately measuring the phosphorus-deuterium distance via 31 P{2 H} rotational echo adiabatic passage double resonance (REAPDOR), it is essential to take the secondary dipolar coupling of 31 P with the boron-bonded 2 H nuclei explicitly into consideration, by simulating a 2 HP -31 P-2 HB three-spin system based on structural input. All of the experimental NMR interaction parameters are found in excellent agreement with values calculated by DFT methods, using the geometries obtained either by energy optimization or from single-crystal structures.
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