by the Laboratory of Microanalysis and Automation of Analytical
Methods (Polish Academy of Science, Łꢃd z´ , Poland) using a Euro-
Vector 3018 analyzer.
count in Gaussian analysis of their high intensities (e equals about
1000m cm ).
ꢀ
1
ꢀ1
Thus, for ligand-field interpretation of [Ni(salpn)], Gaussian analysis
should be use for the visible and UV regions. All the band maxima
reported here were determined from Gaussian analysis of the ex-
perimental spectral contours. Our calculations take into account all
the transitions that are given by ligand-field theory. The absorption
spectra of the nickel(II) complex and the ligand were fitted for
Gaussian components by using the CFP (Curve Fitting Problem)
The solubility of the nickel(II) complex was investigated in 12
common solvents. It was insoluble in water (H O) and ethylene
2
glycol (EG) but was easily soluble in common solvents such as di-
methyl sulfoxide (DMSO), dimethylformamide (DMF), methanol
(
MeOH), ethanol (EtOH), 2-propanol (iPrOH), acetonitrile (MeCN),
chloroform (CHCl ), acetone (AC), dioxane (DX), and toluene (MBz).
3
[49]
[50]
Solutions of [Ni(salpn)] were prepared by dissolving a weighed
amount of the complex in a suitable solvent. The composition of
the complex species in various solutions was confirmed by conduc-
tance measurements. The molar conductance was measured by
using a microcomputer pH/conductivity meter CPC-551 (Elmetron,
Poland) and a platinum dip electrode CD-2. The infrared spectra
were obtained by using KBr with a Nicolet Magna IR 760 spectro-
photometer. The near-IR spectrum (reflectance) of the solid com-
plex was recorded with a CARY 5E (Varian) spectrophotometer. The
electronic spectra of the ligand and nickel(II) complex solutions
were recorded with a SPECORD M40 (Zeiss Jena) spectrophotome-
ter about 15 min after dissolution. The measured spectra of the
computer program. This program is based on the Slavi cˇ nu-
merical algorithm, which for the last few years has successfully
been applied by us for the resolution of d–d (ligand-field) spec-
[30a,51,52]
tra.
Our calculations of the CFM (crystal field model) and
AOM (angular overlap model) parameters were performed for the
II
Ni complex in different solutions by the LFP (Ligand Field Parame-
[53]
ters) program that uses two minimization techniques: the Powell
method (nongradient) and the Davidon–Fletcher–Powell method
(gradient estimation). The AOM calculations were performed within
the framework of the angular overlap simple model developed by
[
54,55]
[56]
Schꢄffer
and Jørgensen. For the CFM calculations, the full
[57]
energy matrices reported by Perumareddi were adopted in the
LFP program. For AOM calculations, the matrix elements of the ex-
cited states given by Hitchman were used, and the one-electron
orbital energies given by Hitchman were adopted. For the four-
coordinate nickel(II) complexes (low-spin, d electronic configura-
ꢀ1
solutions were recorded digitally (20 cm step) over the range of
ꢀ
1
[58]
v=11000 to 50000 cm at room temperature. The measurement
[59]
conditions for the conductivity were the same as those for the
ꢀ
3
8
electronic absorption spectra (i.e., c ꢁ1.0ꢂ10 m). The UV/Vis
spectra were resolved into Gaussian components and were used
to study the solvatochromism and to calculate the chromaticity co-
ordinates as well as the ligand-field (CFM/AOM) parameters.
1
tion, and D4h symmetry), the ground state is A , and a total of 18
1g
d–d transitions were predicted by the CFM (11 spin allowed and 7
spin forbidden). All calculations were performed on an IBM micro-
computer.
The solvent parameters, the Kosower parameter (Z), the Dimroth–
Reichardt parameter [E (30)], the Kamlet and Taft parameters (a, b,
T
p*), dielectric constant (e), and Gutman’s donor and acceptor num-
[36–41]
bers, were obtained from the literature.
Solvent effects could
Conflict of Interest
be the cause of both energy shifts of the absorption bands and
changes in the solution color. The latter effect can be difficult to
observe by the human eye. To characterize the color precisely, tris-
The authors declare no conflict of interest.
[42–45]
timulus colorimetry is usually used.
The chromaticity coordi-
nates were calculated from the absorption spectra (in the region of
Keywords: chromaticity · ligand-field parameters · nickel ·
Schiff bases · solvatochromism
[43,46]
l=380 to 780 nm) by the method described in the literature
for nonuniform (CIE) and two uniform (CIELAB and CIELUV) spaces
[47]
by using the CIEC computer program. This one is designed to
calculate the color parameters for the solution, solid (reflectance),
and simulated spectra. The CIE tristimulus values (X, Y, Z) expressed
[
[
1] P. Przybylski, A. Huczynski, K. Pyta, B. Brzezinski, F. Bartl, Curr Org Chem.
009, 13, 124–148.
2
[43,46]
as integrals
were calculated as were the chromaticity coordi-
nates (x, y, z) and two-space parameters: CIELAB (L*, a*, b*) and
[42,48]
CIELUV (L*, u*, v*). The standard data
were built in the routine,
that is, color matching functions taken every 5 (or 1) nm in the
range of l=380 to 780 nm, as well as standard illuminance D .
65
[
The absorption spectrum was transformed into the equivalent
transmission spectrum.
[
[
6] S. Samadhiya, A. Halve, Orient. J. Chem. 2001, 17, 119–122.
7] M. Alias, H. Kassum, C. Shakir, J. Assoc. Arab Univ. Basic Appl. Sci. 2014,
1
5, 28–34.
[
Method of Calculations
Interpretation of the electronic spectra of the low-spin tetradentate
Schiff base–nickel(II) complex was difficult for several reasons:
[9] D. N. Dhar, C. L. Taploo, J. Sci. Ind. Res. 1982, 41, 501–506.
[
1
) mutual overlapping of the low-symmetry components in the
visible region (tetragonal splittings were not large enough in com-
parison with the spectral band widths); 2) overlapping more inten-
sive CT [or intramolecular (IM)] bands in the near-UV region on d–
d transitions in the visible region; because of this, the maxima of
the d–d bands are not observed in the experimental curve. Most
d–d transitions occur in the UV region and appear close to the in-
tensive CT (or IM) bands. However, the former were taken into ac-
[
[
13] K. Kurzak, A. Gonciarz, I. Ku z´ niarska-Biernacka, Polish J. Chem. 2005, 79,
47–56.
[
[15] K. H. Chjo, B. G. Jeong, J. H. Kim, S. Jeon, C. P. Rim, Y. K. Choi, Bull.
Korean Chem. Soc. 1997, 18, 850–856.
&
ChemistryOpen 2018, 00, 0 – 0
10
ꢀ 2018 The Authors. Published by Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
ÝÝ These are not the final page numbers!