S. Lohar et al. / Tetrahedron Letters 55 (2014) 174–176
175
Figure 1. Proposed mechanism of histidine sensing with TARDHD.
TARDHD shows peaks at 1730, 1691 and 1615 cmꢀ1 corresponding
to carbonyl stretching from aldehyde, ketone and imine (CH@N)
functionalities.
Figure 3. 1H NMR spectral changes of TARDHD upon gradual addition of histidine:
(A) free TARDHD, (B) TARDHD in MeOD + 0.5 equiv histidine in D2O, (C) TARDHD in
MeOD + 1 equiv histidine in D2O, (D) TARDHD in MeOD + 2 equiv histidine in D2O.
In Schiff base adduct (Fig. S7, ESI), 1730 cmꢀ1 peak disappears
with the appearance of a new broad peak at 3386 cmꢀ1, assigned
to imidazole N–H stretching of histidine residue.
The binding constant of TARDHD for histidine is 3.7 ꢁ 104 Mꢀ1
(Fig. S8, ESI), as estimated using the following Benesi–Hildebrand
equation:18
and Fig. S12, ESI). This indicates that neither hydrogen bonding
nor Schiff base formation is individually responsible for fluores-
cence enhancement. Their combined effect is essential for turning
on the fluorescence via ring opening of TARDHD.
À
Á
n
Interaction between TARDHD and histidine has been monitored
by 1H NMR titration in D2O/CD3OD = 1:9 (v/v) (Fig. 3). The alde-
hyde proton at 9.85 ppm of free TARDHD disappears upon addition
of 1 equiv histidine indicating Schiff base formation. Imine proton
(CH@N) of free TARDHD have shifted from 9.59 to 9.23 ppm and
merges to the new imine proton formed due to Schiff base forma-
tion with histidine. Imidazole ring N–H proton, exchangeable with
D2O does not appear, however, imidazole ring –CH2 and –N@CH
protons which generally appear at 7.12 ppm and 8.08 ppm in free
histidine have been shifted to 7.23 and 8.35 ppm upon reaction
with TARDHD.
Density functional theoretical studies (DFT, B3LYP/6-311G basis
set)19 provide additional support to the histidine sensing mecha-
nism. Figure 4 reveals that HOMO–LUMO energy gap in free TARD-
HD and its histidine adduct are 3.107 and 2.695 eV respectively.
Moreover, in HOMO of TARDHD, most of the charge resides in
the rhodamine moiety but in LUMO, it is on the phthalaldehyde
unit. In TARDHD–histidine adduct, most of the charges relocate
on pthalaldehyde unit in both HOMO and LUMO. Most impor-
tantly, it indicates a strong H-bond (2.436 Å) between ketone
oxygen of rhodamine moiety with imidazole N–H from histidine
residue (Fig. 5).
Flim ꢀ F0=FX ꢀ F0 ¼ 1 þ 1=K½Cꢂ
ð1Þ
where F0, Fx and Flim are the emission intensities of TARDHD in ab-
sence of histidine, at an intermediate histidine concentration, and at
histidine concentration of complete interaction respectively. K is
the binding constant, C is the concentration of histidine and n is
the number of histidine molecules bound per TARDHD molecule
(here n = 1). Lowest detection limit for histidine is 1.1 ꢁ 10ꢀ8
M
(Fig. S9, ESI). Figure 2 reveals that TARDHD has no absorbance in
the visible region. In presence of histidine, a new absorption peak
appears at 560 nm, the intensity of which increases with increasing
histidine concentration. This allows naked eye detection and color-
imetric determination of histidine. Figure S10 (ESI) shows UV–vis
titration of TARDHD with histidine which provides the binding con-
stant, 2.8 ꢁ 104 Mꢀ1, in close agreement to the value derived from
fluorescence titration.
The sensing of mechanism is attributed to the formation of
TARDHD–histidine Schiff base followed by its stabilization through
H-bonding involving carbonyl oxygen of rhodamine unit and imid-
azole N–H of histidine residue.
Free imidazole fails to show fluorescence enhancement of
TARDHD. Similarly, other amino acids do not interfere (Figs. S11
Figure 2. Changes of absorbance of TARDHD (10
1, 5, 10, 15, 20, 40, 50, 80, 100, 150, 200, 250, 300, 400, 500, 700, 800, 1000, 2000
and 5000 M) in HEPES buffered (0.1 M) solution (ethanol/water = 1:9, v/v, pH 7.3).
lM) upon addition of histidine (0,
Figure 4. Energy optimized structure and HOMO–LUMO energy gap of TARDHD
and its Schiff base with histidine.
l