ORIGINAL PAPER
How do halogen bonds (S
–
O
⋯
I, N
–
O
⋯
I and C
–
O
⋯
I)
and halogen
–
halogen contacts (C
–
I
⋯
I
–
C, C
–
F
⋯
F
–
C) subsist
in crystal structures? A quantum chemical insight
B. Vijaya Pandiyan
1
&
P. Deepa
2
&
P. Kolandaivel
1
Received: 27 September 2016 /Accepted: 28 November 2016 /Published online: 29 December 2016
#
Springer-Verlag Berlin Heidelberg 2016
Abstract
Thirteen X-ray crystal structures containing various
non-covalent interactions such as halogen bonds, halogen
–
halogen contacts and hydrogen bonds (I
⋯
N, I
⋯
F, I
⋯
I,
F
⋯
F, I
⋯
H and F
⋯
H) were considered and investigated
using the DFT-D3 method (B97D/def2-QZVP). The interac-
tion energies were calculated at MO62X/def2-QZVP and
MP2/aug-cc-pvDZ level of theories. The higher interaction
and dispersion energies (2nd crystal) of
−
9.58 kcal mol
−
1
a n d
−
7 . 1 0
k c a l
m o l
−
1
o b s e r v e d
f o r
1 , 4 - d i -
iodotetrafluorobenzene bis [bis (2-phenylethyl) sulfoxide]
structure indicates the most stable geometrical arrangement
in the crystal packing. The electrostatic potential values cal-
culated for all crystal structures have a positive
σ
-hole, which
aids understanding of the nature of
σ
-hole bonds. The signif-
icance of the existence of halogen bonds in crystal packing
environments was authenticated by replacing iodine atoms by
bromine and chlorine atoms. Nucleus independent chemical
shift analysis reported on the resonance contribution to the
interaction energies of halogen bonds and halogen
–
halogen
contacts. Hirshfeld surface analysis and topological analysis
(atoms in molecules) were carried out to analyze the occur-
rence and strength of all non-covalent interactions. These
analyses revealed that halogen bond interactions were more
dominant than hydrogen bonding interactions in these crystal
structures.
Keywords
Halogen bond
.
Stabilization energy
.
Hirshfeld
surface
.
Nucleus independent chemical shift (NICS)
.
Atoms
inmolecules(AIM)
.
Molecular electrostatic potential(MESP)
map
Introduction
Many scientists nowadays have focused their attention
towards halogen bonds, which play a vital role in crystal
packing. Halogen bonds can stabilize inter- and intra-
molecular interactions in proteins and nucleic acid struc-
tures [
1
], help to form four-stranded DNA junctions [
2
],
transport anions in a lipid layer [
3
], can be used to rec-
ognize anions in fluorescence microscopy [
4
], and play
pivotal role in the interactions of halogen atoms inside a
molecular container [
5
]. For the above reasons, halogen
bonds have been utilized in drug design with increased
efficiency [
6
]. In material engineering, thin film struc-
tures [
7
], liquid crystals [
8
], and gels [
9
,
10
] can be
formed by halogen bonds. Halogen bonds form between
the charge depleted region of a electronegative atom R
–
X (X = Halogen), and charge intense regions (e.g., lone
pairs) [
11
,
12
]. As a result, X continues to be nucleo-
philic in character [
13
] by proceeding as an electron ac-
ceptor, and R
–
X
⋯
B is found to be about 180° [
14
].


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