Following our previous studies of hypervalency in SFn (n = 1-6) and ClFn (n = 1-7), we have characterized the structures and energetics of PFn (n = 1-5) species with RCCSD(T) coupled cluster calculations and triple- and quadruple-ζ quality correlation consistent basis sets. The prior studies demonstrated that hypervalent bonding occurs when it is energetically favorable to uncouple a pair of electrons to form new bonds, a process we describe as recoupled pair bonding. In contrast to S and Cl, ground state P(4S) has no 3p2 pairs that can be recoupled, but the 3s2 pair of all three elements is susceptible to recoupled pair bonding when more energetically accessible bonding pathways have been exhausted. We found that this can first occur when F is added to PF 2(X2B1), which yields PF3(X 1A1) via normal covalent bonding but yields PF 3(a3B1) via recoupled pair bonding. PF 3(a3B1) lies 92.1 kcal/mol above PF 3(X1A1) but is still bound by 42.0 kcal/mol with respect to PF2(X2B1) + F at the RCCSD(T)/aug-cc-pVQZ level. We characterized both of the isomers of PF 4: the more stable and familiar one that has two covalent equatorial bonds and two axial hypervalent bonds (that use both electrons of the recoupled 3s2 pair) and the less-studied one that has three covalent bonds and only one hypervalent bond. The transition state between these two minima was also located. In addition to the states that can be formed from P( 4S), there is another group of low-lying excited state species that can be formed from P(2D) via various combinations of covalent and recoupled pair bonding. Additions of the latter type include PF(B 3Π) formed from P(1D) + F and PF2(B 2B2) formed from either PF(a1Δ) + F or PF(B3Π) + F.
|Original language||English (US)|
|Number of pages||7|
|Journal||Journal of Physical Chemistry A|
|State||Published - Aug 26 2010|
ASJC Scopus subject areas
- Physical and Theoretical Chemistry