Properties of Cationic Pnicogen-Bonded Complexes F<sub>4–<i>n</i></sub>H<sub><i>n</i></sub>P<sup>+</sup>:N-Base
with F–P···N Linear and <i>n</i> =
0–3
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Abstract
Ab
initio MP2/aug′-cc-pVTZ calculations were performed to investigate
the pnicogen-bonded complexes F<sub>4–<i>n</i></sub>H<sub><i>n</i></sub>P<sup>+</sup>:N-base, for <i>n</i> = 0–3, each with a linear or nearly linear F–P···N
alignment. The nitrogen bases include the sp<sup>3</sup> bases NH<sub>3</sub>, NClH<sub>2</sub>, NFH<sub>2</sub>, NCl<sub>2</sub>H, NCl<sub>3</sub>, NFCl<sub>2</sub>, NF<sub>2</sub>H, NF<sub>2</sub>Cl, and
NF<sub>3</sub> and the sp bases NCNH<sub>2</sub>, NCCH<sub>3</sub>, NP, NCOH, NCCl, NCH, NCF, NCCN, and N<sub>2</sub>. The binding
energies vary between −20 and −180 kJ·mol<sup>–1</sup>, while the P–N distances vary from 1.89 to 3.01 Å. In
each series of complexes, binding energies decrease exponentially
as the P–N distance increases, provided that complexes with
sp<sup>3</sup> and sp hybridized bases are treated separately. Different
patterns are observed for the change in the binding energies of complexes
with a particular base as the number of F atoms in the acid changes.
Thus, the particular acid–base pair is a factor in determining
the binding energies of these complexes. Three different charge-transfer
interactions stabilize these complexes. These arise from the nitrogen
lone pair to the σ*P–F<sub>ax</sub>, σ*P–F<sub>eq</sub>, and σ*P–H<sub>eq</sub> orbitals. The dominant
single charge-transfer energy in all complexes is N<sub>lp</sub> →
σ*P–F<sub>ax</sub>. However, since there are three N<sub>lp</sub> → σ*P–F<sub>eq</sub> charge-transfer
interactions in complexes with F<sub>4</sub>P<sup>+</sup> and two
in complexes with F<sub>3</sub>HP<sup>+</sup>, the sum of the N<sub>lp</sub> → σ*P–F<sub>eq</sub> charge-transfer
energies is greater than the N<sub>lp</sub> → σ*P–F<sub>ax</sub> charge-transfer energies in the former complexes, and similar
to the N<sub>lp</sub> → σ*P–F<sub>ax</sub> energies
in the latter. The total charge-transfer energies of all complexes
decrease exponentially as the P–N distance increases. Coupling
constants <sup>1p</sup><i>J</i>(P–N) across the pnicogen
bond vary with the P–N distance, but different patterns are
observed for complexes with F<sub>4</sub>P<sup>+</sup> and complexes
of the sp<sup>3</sup> bases with F<sub>3</sub>HP<sup>+</sup>. These
initially increase as the P–N distance decreases, reach a maximum,
and then decrease with decreasing P–N distance as the P···N
bond acquires increased covalent character. For the remaining complexes, <sup>1p</sup><i>J</i>(P–N) increases with decreasing
P–N distance. Complexation increases the P–F<sub>ax</sub> distance and <sup>1</sup><i>J</i>(P–F<sub>ax</sub>) relative to the corresponding isolated ion. <sup>1</sup><i>J</i>(P–F<sub>ax</sub>) correlates quadratically with
the P–N distance