Ab Initio Design Of Chelating Ligands Relevant To Alzheimer'S Disease: Influence Of Metalloaromaticity - Physical Chemisrty Page 3

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The Journal of Physical Chemistry A
ARTICLE
Information. Geometry optimizations, frequency calculations, and
single-point energy CPCM calculations were performed using
54
the Gaussian 03 set of programs.
As a structure-based measure of metalloaromaticity, we have
calculated the harmonic oscillator model of aromaticity (HOMA)
55,56
index, defined by Kruszewski and Krygowski as
R
n
2
HOMA ¼ 1 À
ðR
À R
Þ
ð1Þ
opt
i
n
i ¼ 1
where n is the number of bonds considered and R is an empirical
constant (for CÀC, CÀN, and CÀO bonds R = 257.7, 93.5 and
157.4, respectively) fixed to give HOMA = 0 for a model
nonaromatic system, and HOMA = 1 for a system with all bonds
equal to an optimal value R
(1.388, 1.334, and 1.265 Å for
opt
CÀC, CÀN, and CÀO bonds, respectively), assumed to be
achieved for fully aromatic systems. R
stands for a running bond
i
length. The calculated HOMA values correspond to the
OCCCN group of atoms of the metallacycle, that is, all pairs of
atoms present in the metalated ring except NÀCu and OÀCu
and R values for these bonds are not available. In
because R
opt
addition, the electronic-based I
index (which estimates the
NG
cyclic overlap of molecular orbitals in a given ring) has also been
calculated for some of the compounds by obtaining the corre-
sponding wave functions of the compounds under analysis. If we
consider a ring structure of N atoms represented by the following
string A = {A
}, for a closed-shell monodeterminantal
, A
, ..., A
1
2
N
wave function, then the multicenter I
index, a normalized
NG
57,58
59
version of Giambiagi’s
I
, reads
ring
ðA Þ
I
NG
π
2
occ:MO
¼
½2
N
ðA
ÞS
ðA
Þ 3 3 3 S
ðA
ÞŠ
1=N
n
n
3 3 3 n
S
i
i
1
i
i
2
i
i
N
i
i
i
1
N
2
3
N
1
4NN
2
1
2
π
i
, i
, 3 3 3 , i
1
2
N
ð2Þ
ÀOHn and
Figure 1. Optimized structures of the chelating ligands (N
X
is the number of π-electrons, S
where N
(A) is the overlap
π
NÀOH4) and of the Cu(II) complexes ([Cu(N
-On)
] and
ij
X
2
between natural orbitals i and j in the atom A, and n
are their
[Cu(NÀO4)
]). X = NH, O, and S; n = 1À3.
i
2
value is ∼0.04.
60
occupancies. For benzene, the I
Although
NG
76
several atomic partitions may be used for the calculations of the
used.
The total complexation energy (ΔE) corresponds to the
À
2+
overlap between molecular orbitals i and j within the molecular
reaction of Cu
+ 2 L
f [Cu(L
)] (L being the chelating
2
61,62
space assigned to atom A,
we have chosen in the present work
ligands), and through EDA it is decomposed into two terms, the
preparation and the interaction energies: ΔE = ΔE
+ ΔE
the partition carried out in the framework of the quantum theory of
.
prep
int
63,64
atoms-in-molecules (QTAIM) of Bader,
by which atoms are
The preparation energy (ΔE
) is the amount of energy
prep
defined from the condition of zero-flux gradient in the one-electron
required to deform the ligands from their equilibrium structure
density, F(r). Calculation of atomic overlap matrices (AOMs) and
to the geometry that they acquire in the metal complex, whereas
65
computation of I
have been performed with the AIMPAC
and
the interaction energy (ΔE
) corresponds to the actual energy
NG
int
66
ESI-3D
collection of programs. For the I
calculations, all atoms
change when these geometrically deformed ligands are combined
NG
with Cu to form the metal complexes. ΔE
present in the metal ring including the Cu atom have been
is analyzed in the
int
considered. For the indices used, it is established that the higher
framework of the KohnÀSham molecular orbital model using a
the HOMA and the I
values the more aromatic the rings.
quantitative decomposition of the bond into electrostatic interaction,
NG
Moreover, to get a better understanding of the bonding
Pauli repulsion, and orbital interactions terms represented as
ΔE
= ΔV
+ ΔE
+ ΔE
. ΔE
between Cu(II) and the chelating ligands, an energy decomposition
can be decomposed
int
elstat
Pauli
oi
oi
67À73
70,71
analysis (EDA) has also been carried out.
The Amsterdam
according to the extended transition-state method (ETS)
74
into the contributions from each irreducible representation Γ of
density functional (ADF)
software has been used for such
purpose, and the EDA analysis has been calculated onto the
the interacting system. In the planar systems, we have performed
the σ/π separation because this symmetry partitioning has been
B3LYP/[10s7p4d1f]-ECP-6-31++G(d,p) ECP optimized geo-
metries by a single-point energy calculation with the B3LYP
proven to be quite informative.
39,40
functional
using the TZ2P basis set that contains an uncon-
tracted set of Slater-type orbitals (STOs) of triple-ζ (TZP)
’ RESULTS AND DISCUSSION
quality with diffuse functions and two sets of polarization
75
functions.
To reduce the computational time needed to carry
Geometries, Reaction Energies, and Stability Constants.
out the calculations, the frozen core approximation has been
As mentioned, metal-ion chelators considered in the present
12661
|J. Phys. Chem. A 2011, 115, 12659–12666

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