4
J.C. Truscott et al. / Journal of Molecular Structure xxx (xxxx) xxx
Table 1
Experimental details.
Crystal Data
1a- [Ga(L1)(H
70Ga
2
O)
2
].NO
3
þ EtOH
1b - [Ga(L1)(OSMe
2
)
2
].NO
3
þ OSMe
2
Chemical formula
C
54
H
2
N
6
O
21
C
30
H
40GaN
3 10 3
O S
M
r
1282.63
768.55
Crystal system, space group
Temperature (K)
Triclinic, P-1
100
Triclinic, P-1
100
a, b, c (Å)
12.081 (5), 13.090 (5), 19.471(5)
91.044 (5), 90.158(5), 112.947(5)
2834.8 (18)
2
10.194(3), 11.686(4), 15.796(5)
111.335(10), 92.429(12), 90.716(11)
1750.5 (10)
2
ꢁ
a
,
b
,
g
( )
3
V (Å )
Z
Radiation type
Mo K
1.04
a
Mo Ka
1.02
ꢀ
1
m
(mm
)
Crystal size (mm)
Data collection
0.47 ꢂ 0.27 ꢂ 0.14
0.45 ꢂ 0.15 ꢂ 0.1
Diffractometer
Absorption correction
No. of measured, independent and observed
Bruker APEX-II CCD
None
41 255, 12 745, 7332
Bruker APEX-II CCD
None
27 419, 8461
[I > 2s(I)] reflections
R
int
0.067
0.102
0.053
0.109
(
sin
q/l)
max (Åꢀ1)
Refinement
2
2
2
R [F > 2
s(F )], wR (F ), S
0.128, 1.454, 1.02
0.118, 0.274, 0.112
No. of reflections
No. of parameters
No. of restraints
H-atom treatment
12 745
741
3
8461
440
18
H atoms treated by a mixture of independent and
constrained refinement
3.79, ꢀ2.51
H atoms treated by a mixture of independent and
constrained refinement
2.14, ꢀ1.77
Drmin (e Å 3
ꢀ
)
Drmax
,
2
.4. Computational method
optimized using density functional theory calculations. Both DFT
PW91/TZP gas phase optimized isomers are non-planar. L1 Isomer
1, which exhibits the same orientation as the experimental struc-
ture, has the lowest energy, see Fig. 2 a. The energy of L1 isomer 2 is
too high to exist, since when applying the Boltzmann equation to
the energies of L1 isomer 1 and L1 isomer 2, a population of 99.99
and 0.01% for the two isomers respectively, are obtained. L1 Isomer
1 has the correct orientation for tetradentate coordination with a
metal. Upon coordination to gallium (III) an octahedral complex is
formed. Since Ga(III) prefers to be six coordinated, two water
molecules that are available in the reaction mixture, fill the axial
DFT calculations were carried out in the gas and solvent phase
with the PW91 (Perdew-Wang 1991) [16] GGA (Generalized
Gradient Approximation) functional and the all-electron Slater-
type TZP (Triple
z
polarized) basis set as implemented in the ADF
Amsterdam Density Functional) 2014 programme and updates
17], and with the B3LYP functional using the triple- basis set 6-
11G (d,p) as implemented in the Gaussian 09 package [18]. The
(
[
3
z
implicit solvent Polarizable Continuum Model (PCM) [19] that uses
the integral equation formalism variant (IEFPCM) [20] was used for
solvent calculations in Gaussian and the COSMO (Conductor like
Screening Model) model of solvation [21e23] as implemented [24],
was used for solvent calculations in ADF. The type of cavity used is
Esurf [25] and solvent used was DMSO with ε ¼ 46.7 or ethanol
positions to complete the octahedral coordination. The DFT PW91/
þ
TZP optimized geometry of gallium complex 1a, [Ga(L1)(H
2
O)
2
] , is
.
2 2 3
shown in Fig. 3. However, when [Ga(L1)(H O) ] NO is dissolved in
DMSO, the axial waters are replaced by DMSO to form gallium
.
(
EtOH) with ε ¼ 24.55. The input coordinates for the compounds
complex 1b, [Ga(L1)(OSMe
geometry of [Ga(L1)(OSMe
2
)
)
2
] NO
3
. The DFT PW91/TZP optimized
þ
were constructed using Chemcraft [26], as well as available crystal
data. The optimized coordinates of the DFT calculations are pro-
vided in the Supporting Information.
2
2
] , is also shown in Fig. 3.
The tetradentate N4 carboxamide ligand L2 was synthesized by
adapting a published method for the unsubstituted ligand N,N’-
(
1,2-phenylene)bis (pyridine-2-carboxamide), L2a, from literature
[15]. A published crystal structure of the unsubstituted ligand L2a
CSD reference code GUKWEO [30]) showed that the both pyridine-
3
. Results and discussion
(
3
.1. Synthesis and structure
2-carboxamide groups are orientated in the same direction (similar
as in Fig. 2 b, L2a isomer 1), stabilized by a hydrogen bond between
the carboxamide oxygen and an amine hydrogen. This orientation
is unfavourable for N4 e coordination to a metal. However, PW91/
TZP density functional theory calculations of the two possible ste-
reo isomers of L2a (Fig. 2 b) showed that these two isomers are near
iso-energetic, with a Boltzmann calculated population of 25.6 and
74.4% for L2a isomer 1 and L2a isomer 2, respectively. Thus both
orientations are possible. A similar result was obtained for the three
possible isomers of L2, see (Fig. 2 d). Experimentally both isomers
of the 4,5-dimethyl substituted ligand, 4,5-dimethyl-1,2-phenylene
L2b were isolated in the solid state (CSD reference codes AVURIS
and QEDFEM [4,31]). Consistent with experimental observation, the
PW91/TZP energies of L2b isomer 1 and L2b isomer 2 are also near
iso-energetic (Fig. 2 c), with a Boltzmann calculated population of
33.0 and 67.0%, respectively. Isomer 2 of L2, L2a and L2b has the
The tetradentate Schiff base ligand L1 is synthesized by the ball
milling assisted solvent and catalyst free method, where the re-
actants ortho-vanillin and 4,5-dimethyl-1,2-phenylendiamine were
shaken at a high speed in the absence of solvent inside a vessel
containing grinding balls. The high speed produces enough force to
facilitate the chemical reaction which makes an amorphous
mixture of the reagents [27]. The reason for the use of ball milling
over conventional methods of chemical synthesis, is to enable a
chemical reaction in the absence of solvents, resulting in a cleaner
synthetic procedure [28]. The solid-state structure of L2 is known
(
CSD reference code PUJGIL [29]). The L2 free ligand in the solid
state deviates severely from planarity due to the repulsion between
the hydroxy and methoxy groups and has the structure of L1 isomer
1
in Fig. 2 a. The two different stereo isomers possible for L1, are
Please cite this article as: J.C. Truscott et al., Synthesis, structure and DFT study of novel Ga(III) complexes containing a tetradentate ligand,