The packing of molecular crystals,
in which the constituent molecular
units have no directional forces, is primarily controlled by weak
London dispersion (LD) forces. These forces assist in stabilizing
the system by bringing the molecular units into the proximity of each
other. In this paper, the same effect is shown to be externally induced
by pressure. The minimal pressure required to correctly describe the
crystal structure without LD interactions (P
LD) provides a quantifiable measure for the weak intermolecular
interactions. LD forces are shown to be essential for an accurate
description of the pressure-induced phase transitions across examples
of linear, trigonal-planar, square-planar, tetrahedral, trigonal bipyramidal,
and octahedral molecules.
Iron carbonyls are known to form
18-electron complexes like Fe(CO)5, Fe2(CO)9, and Fe3(CO)12 having terminal or bridged
Fe–CO bonding. Based on
genetic algorithm-assisted density functional theory (DFT) calculations,
it is predicted that at pressures above 2 GPa, iron tetracarbonyl,
Fe(CO)4, attains a square-planar geometry with a 16-electron
count. Compression overcomes the [Ar]4s23d6 (S = 2) → [Ar]4s03d8 (S = 0) excitation energy to stabilize a closed-shell Fe(CO)4 with a d8-configuration. Strong σ(4CO) →
Fe (d
x
2
–y
2) bonding along with Fe(d
xz
, d
yz
) and Fe(d
xy
) → π (CO)4* back-bonding
assists the formation of square-planar Fe(CO)4 under pressure.
Compression progressively flattens and destabilizes the ambient pressure
C2v structure of Fe(CO)4, and beyond 2 GPa,
it undergoes a sharp C2v → D4h transition
with ΔV
unit‑cell = 2.1% and trans-θ(OC–Fe–CO) = 180°. Realizing
a square-planar geometry in a four-coordinated Fe-carbonyl complex
shows the rich prospects of the new chemistry under pressure.
A conformationally flexible ligand [(Flu)-(CH2)2-(NHC)-CH2-(NHC)-(CH2)2-(Flu)]2- (L) is devised that offers four sequential organic donors modules and enwraps a Ca2+ pseudo-tetrahedrally in a twisted ‘S’-shape. The [(L)Ca] synthesis is intriguingly stepwise...
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