V.T. Kasumov, E. Sahin / Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy 107 (2013) 31–38
33
precipitated red complex was collected by suction filtration and
washed with water, could methanol and recrystallised from meth-
anol/chloroform mixture. The synthesis of complexes 11 and 12
was carried out in the same way as that described for above com-
plexes, but 10 ml glacial acetic acid was used instead of acetoni-
trile. The crude orange red solid complexes 11 and 12 were
recrystallized in methanol/CHCl3 mixture.
Theelectronic spectra of 1–6(Table 1, Figs. 1 and 2a), unlikemany
other non-fluorinated bidentate arylsalicylaldimines [20,27,28], did
not exhibit absorptions above 370 nm even in the concentrated
strongly H-bonding polar solvents such as ethanol and methanol
solutions. This observation suggests that the perfluorinated 1–6 sal-
icylaldimines exist only in enol-imine tautomer form at room tem-
perature. The higher intense absorption bands observed in the
ranges of 210–330 and 355–362 nm (Table 1) have been assigned
to
p ?
pꢄ and n ? pꢄ transitions for the electrons localized on the
Hydrogenation procedure
aromatic and imine groups, respectively. However, a more intense
band at 355–362 nm, according to their higher extinction coeffi-
The hydrogenation of nitrobenzene was carried out in a thermo-
static reaction flask (100 ml) at 25 °C under 760 Torr H2 with vig-
orous stirring in dry and deoxygenated 25 ml DMF solution.
Catalyst (1.0 ꢁ 10ꢂ5 to 4.0 ꢁ 10ꢂ6 mol) was added into 25 ml
DMF and saturated with H2 for 10–15 min. After addition of NaBH4
(5 ꢁ 10ꢂ6 mol) the mixture was stirred for ca. 5 min and PhNO2 (4–
8 ꢁ 10ꢂ4 mol) was transferred into the vessel. Then the H2 gas was
bubbled again into the flask and the volume of the absorbed H2
was measured periodically.
cients (e
= 10,000–39,000 Mꢂ1cmꢂ1) can be assigned to overlapped
bands originated from low intense n ? pꢄ transitions and higher in-
tense charge transfer absorptions [28]. Thus, UV/Vis study in the dif-
ferent solvents indicates that no tautomerisim takes place in polar
Table 1
Electronic spectral data for 1–12 and their oxidized intermediates.
Compound Solvent
Electronic spectra, k (nm), (loge )
, Mꢂ1 cmꢂ1
1
MeOH
MeCN
207(4.83), 222*, 235*, 277(4.35), 325*, 356(4.21)
222(4.6), 235**, 277(4.4), 309(4.12), 322 (4.1)*,
355(3.98)
X-ray crystallography
MeCN + Ox. 222, 275, 308, 320*, 354, 520*
MeOH
For the crystal structure determination, the single-crystals of
the complexes (12ꢃCHCl3) were used for data collection on a
four-circle Rigaku R-AXIS RAPID-S diffractometer (equipped with
a two-dimensional area IP detector). The graphite-monochroma-
2
208(4.7), 220(4.6), 281(4.5), 314(4.5), 329*,
360(4.3)
EtOH
MeCN
210(4.8), 224(4.8), 237*, 281(4.7), 331*, 362(4.3)
221(4.5), 235*, 280(4.4), 314(4,4), 329*, 358(4.2)
MeCN + Ox. 268, 285*, 315, 328*, 350
tized Mo K
nique with
a
D
radiation (k = 0.71073 Å) and oscillation scans tech-
= 5° for one image were used for data collection.
3
4
MeOH
208(4.9), 227(4.8), 276(4.8), 305(4.4), 321(4.6),
x
356(4.5)
The lattice parameters were determined by the least-squares
EtOH
218*, 233(4.9), 276(4.8), 306(4.7), 320(4.6), 357
(4.5)
methods on the basis of all reflections with F2 > 2 (F2). Integration
r
of the intensities, correction for Lorentz and polarization effects
and cell refinement was performed using Crystal Clear (Rigaku/
MSC Inc., 2005) software [25]. The structures were solved by direct
methods using SHELXS-97 [26] and refined by a full-matrix least-
squares procedure using the program SHELXL-97 [26]. H atoms
were positioned geometrically and refined using a riding model.
The final difference Fourier maps showed no peaks of chemical
significance.
MeCN
MeCN + Ox
MeOH
227(3.3),276(3.2), 305(3.1), 320(3.1), 355(2.9)
272, 308, 320*, 352, 420*, 520*
207(4.8), 222(4.7), 236**, 282(4.6), 306(4.6),
323*, 358(4.6)
MeCN
223(4.6), 333**, 282(4.47), 306(4.5), 322*,
357(4.3)
MeCN + Ox. 278, 305, 320*, 355, 550**
MeOH
MeCN
MeCN + Ox
MeOH
5
6
206(4.6), 231(4.5), 278(4.4), 305(4.3), 361(4.1)
229(4.5), 280(4.4), 306*(4.33), 321**, 360(4.1)
230*, 277, 305*, 322*, 355, 715
206(4.8), 225(4.8), 279(4.7), 300(4.6), 322*,
361(4.4)
224(4.46), 279(4.34), 323*(4.19), 360(4.05)
277, 304*, 322*, 736
Results and discussion
MeCN
MeCN + Ox
EtOH
CHCl3
MeCN
7
8
208(4.6), 239*(45), 263(4.6), 303(4.3), 414(3.7)
263(4.8), 306(4.5), 414(3.9)
IR and UV/visible spectroscopic characterization of 7–12 compounds
241(4.93), 262(4.98), 302(4.65), 409(4.19)
The analytical, IR, 1H NMR spectroscopic characteristics of the
compounds 1–6 were previously reported [8–10,13]. The analyti-
cal, IR, 1H NMR spectroscopic characteristics of the compounds
7–12 is presented in Supplemental part. In order to compare the
spectral properties of the ligands and their 7–12 complexes, also
we have measured the IR and 1H NMR characteristics of 1–6 li-
gands. The IR spectra of all compounds exhibit sharp bands in
the region of 2860–2950 cmꢂ1 due to the asymmetric and sym-
MeCN + Ox
EtOH
235*, 289, 350, 404*, 530**
210(4.5), 237(4.6), 264(4.6), 303(4.3), 353*(4.2),
420(4.2)
CHCl3
MeCN
MeCN + Ox
EtOH
CHCl3
MeCN
MeCN + Ox
EtOH
CHCl3
MeCN
MeCN + Ox
EtOH
CHCl3
MeCN
MeCN + Ox
EtOH
CHCl3
MeCN
MeCN + Ox
261(4.97), 306(4.62), 421(4.08)
238(4.5), 262(4.6), 303(4.28), 416(3.7)
250*, 294, 320*, 378, 405
9
10
11
12
219(4.7), 252(4.0), 301(4.9), 354(3.3), 422(3.4)
259(4.17), 305(3.91), 358*(3.10), 422(3.56)
220(4.5), 262(4.54), 302(4.3), 416(3.72)
237, 261*, 296, 355*, 413, 530**
237*(4.52), 263(4.55), 302(4.26), 417(3.78)
262(4.83), 306(4.76), 420(4.09)
240*(4.1), 262(4.13), 302(3.98), 414(3.47)
234*, 294, 348*, 404* 500**
240(4.77), 260(4.89), 304(4.48), 430(3.98)
258(3.62), 307(4.67), 432(4.03)
240(4.57), 261(4.86), 305(4.57), 426(4.06)
238*, 296, 355*, 419
metric
m(CAH) stretching frequencies of the C(CH3)3 groups. The
m
(C@N) stretching vibrations of 7–12 are blue shifted (1602–
1616 cmꢂ1
) relative to those of free 1–6 ligands (1622–
1630 cmꢂ1), indicating coordination of the imine nitrogen atom
to copper(II) (Section ‘Experimental’). A weak broad feature cen-
tered at 2500–2800 cmꢂ1, due to
m(OH) of the intramolecularly
H-bonded OHꢃ ꢃ ꢃN in 1–6, disappears in the spectra of all the com-
plexes. This suggests their coordination via deprotonated phenolic
oxygen atom to Pd(II). The appearance of new bands at 1526–
208(4.7), 241(4.9), 262(4.9), 306(4.7), 430(4.2)
269(4.9), 308(4.8), 430(4.2)
240(4.8), 261(4.9) 305(4.5), 426(4.0)
231, 299, 355, 419
1530 cmꢂ1, attributable to the coordinated
m(CAO) stretching
mode [27,28] and in the 450–660 cmꢂ1 region assignable to the
PdAO and PdAN bonds, further confirmed the coordination of li-
gands through phenolic O and azomethine N atoms.
*
Shoulder.
Very weak shoulder.
**