M. Saikiran et al. / Dyes and Pigments 140 (2017) 6e13
9
3
1
1
(
1),
694-s (C¼O), 1604-s (C¼ C), 1515-s (C¼ C (Ar)), 1417-s (CH
365-m (C-N), 1316-w (C-O), 833-w (P-substitution), 782-m 714-s
C-H (oop)).
-butyl-2-((1E,3E,5E)-7-((E)-1-butyl-5-carboxy-3,3-
d
13.78 (C-32),
d
13.56 (C-28). FTIR (KBr, cmꢁ1): 2958-m (OH),
bend),
2
1
dimethylindolin-2-ylidene)hepta-1,3,5-trien-1-yl)-5-hydroxy-3,3-
dimethyl-3H-indolium chloride (UCD-2) obtained in 5% yield. (HR)-
ESI - TOF mass (measured 553.3415 [M] þ; calculated 553.3425). 1H
NMR (500 MHz CDCl3): 0.97 (6 H, t),1.12e1.58 (8 H, m), 1.65 (6 H, s),
1
.69 (6 H, s), 3.99 (2 H, m), 4.44 (2 H, m), 6.10e6.99 (7 H, m), 7.2 (3 H,
13
m), 7.99 (2 H, m), 8.33 (1 H, s). C NMR (125 MHz, DMSO:
C-17), 170.09 (C-9), 166.18 (C-1), 153.49 (C-6), 149.34 (C-24),
144.94 (C-19), 140.79 (C-5), 132.49 (C-15), 131.75 (C-
1,12,13,14), 129.92 (C-3, 22), 126.99 (C-7), 123.57 (C-21),
122.11 (C-20), 120.89 (C-2), 104.77 (C-23), 98.67 (C-4), 95.74
C-10), 93.05 (C-16), 58.26 (C-18), 48.73 (C-25), 44.34 (C-8),
42.38 (C-29), 29.69 (C-26), 28.22 (C-30), 25.54 (C-33), 24.80
20.41 (C-27), 20.16 (C-31), 15.29 (C-32), 14.55 (C-28).
d177.17
(
d
1
d
(
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
d
Fig. 1. Electronic absorption (solid line) and fluorescence emission (dashed line)
spectra of UCD 1-3 in DMF solution (5 mM).
(
C-34),
d
d
d
d
FTIR (KBr, cm-1): 2964-m (OH), 1695-m (C¼O),1605-s (C¼ C), 1521-
m (C¼ C (Ar)), 1417-m (CH2 bend), 1360-s (C-N), 1291-w (C-O
present in main
p-conjugated polymethene framework. The lmax of
(
carboxyl)), 1091-s (C-O), 831-w (p-substitution), 716-s (m-substi-
unsymmetrical cyanine dyes ranges from 764 to 774 nm with high
molar extinction coefficients (ε z 10 dm M cm ). This sharp
and intense light absorption in this class of dyes is associated with
tution), 658-w (C-H (oop)).
-butyl-2-((1E,3E,5E)-7-((E)-1-butyl-5-carboxy-3,3-
dimethylindolin-2-ylidene)hepta-1,3,5-trien-1-yl)-5-iodo-3,3-
dimethyl-3H-indolium chloride (UCD-3) obtained in 11% yield. H
NMR (500 MHz CDCl ): 0.97 (6 H, t), 1.1e1.58 (8 H, m), 1.65 (6 H, s),
.69 (6 H, s), 4.0e4.10 (4H, m), 6.2e7.2 (7 H, m), 7.55 (1 H, s), 7.63
5
3
ꢁ1
ꢁ1
1
1
the
for each of dyes were measured slightly below (about 15e20 nm) to
the corresponding max of absorption spectrum as the excitation
pꢁ
p* electronic transitions. The fluorescence emission spectra
3
l
1
13
wavelength. For all of the unsymmetrical cyanine dyes one main
emission band can be observed which is ranging from 788 nm to
(
2 H, d), 7.99 (1 H, s), 8.09 (2 H, d). C NMR (125 MHz, DMSO:
176.20 (C-17), 173.70 (C-9), 168.09 (C-1), 154.23 (C-5), 147.10
C-24), 146.47 (C-19), 145.07 (C-6), 140.91 (C-15), 133.14 (C-14),
132.69 (C-13), 131.68 (C-12), 129.62 (C-11), 125.78 (C-7),
124.06 (C-3, 22), 123.70 (C-21), 122.37 (C-20), 121.87 (C-2),
119.29 (C-23), 113.63 (C-4), 112.14 (C-10), 86.92 (C-16), 69.18
63.35 (C-25), 48.29 (C-8), 44.65 (C-29), 29.89 (C-26),
29.87 (C-30), 27.98 (C-33), 24.44 (C-34), 20.36 (C-27), 20.13
14.35 (C-32), 14.20 (C-28). FTIR (KBr, cm ): 2958-m (OH),
d
(
d
d
d
d
d
d
d
798 nm, with a small Stokes shift of 23 and 24 nm. This small Stokes
d
d
d
d
d
d
shift represents the rigidity of the molecules without having any
conformational changes after the photoexcitation.
To investigate the interactions between the dyes and the bio-
molecules for imaging applications, Phosphate buffer solution
d
d
d
d
d
d
d
d
(
C-18),
d
d
d
d
(
PBS) has been most commonly used. Keeping this in mind, elec-
tronic absorption spectra of these dyes were also measured in the
.1 M PBS solution at pH 7.4 which has been shown in Fig. 2. It is
worth mentioning that the absorption spectra of cyanine dyes in
PBS exhibited slightly blue shifted max compared to that observed
in DMF. This behaviour of blue shifted max could be attributed to
d
d
d
d
d
ꢁ1
(
C-31),
d
d
0
1
699-m (C¼O), 1605-m (C¼ C), 1506-s (C¼ C (Ar)), 1415-s (CH
2
bend), 1360-s (C-N), 1309-w (C-O (carboxyl)), 816-w (p-substitu-
tion), 714-s (m-substitution), 649-m (C-H (oop)), 554-w (C-I).
l
l
the enhancement in aggregation of dye, promoted by the hydrogen
bonding between the dye molecules due to the presence of eCOOH
groups. It is well known that cyanine dyes exhibit dye aggregation
3
. Results and discussion
3.1. Photophysical characterization
owing to their flat molecular structure [32]. Apart from the main
p-
p
* electronic transition, cyanine and squaraine dyes also exhibit a
After the successful synthesis and purification these NIR sensi-
vibronic shoulder just before the main absorption peak and the
vibronic shoulder has been reported to be marker of molecular
aggregation [33]. Higher value of the ratio of absorbance for the
vibronic shoulder with respect to the absorbance corresponding to
tive dyes were subjected to photophysical investigations pertaining
to the electronic absorption and fluorescence emission spectros-
copy. Results thus obtained pertaining to the photophysical pa-
rameters have been summarized in Table 1. Fig. 1 exhibits the
solution state electronic absorption and fluorescence emission
spectra for the unsymmetrical cyanine dyes in the dime-
thylformamide (DMF) solution.
It can be observed that position of absorption maxima (lmax) for
the electronic absorption and fluorescence emission in DMF are not
much affected by the different substituents (hydroxyl and iodo)
the main
34,35].
A perusal of absorption spectra shown in Fig. 2 clearly corrob-
p-p* transition indicates an enhanced dye aggregation
[
orates that vibronic shoulders of the dyes in PBS are relatively more
pronounced as compared to that observed in the DMF (Fig. 1)
verifying the enhanced dye aggregation and this could be
Table 1
Spectral properties of dyes in DMF and 0.1 M PBS solution at pH 7.4.
Dye
DMF Solution
(max) Absorption
PBS Solution
(max) Absorption
Quantum Yield
(ε) (dm3
M
ꢁ1
ꢁ1
cm )
l
l
l
(max) Emission
Stoke Shift
5
UCD -1
UCD -2
UCD -3
764 nm
769 nm
774 nm
788 nm
792 nm
798 nm
24 nm
23 nm
24 nm
1.1 ꢀ 10
0.8 ꢀ 10
1.4 ꢀ 10
749 nm
753 nm
757 nm
0.327
0.196
0.649
5
5