podand 2 with N, S donors showed the highest FE. Podand 4
with Se, N donors and long alkyl chains showed enhanced
visual selectivity for Fe(II). The fluorenoazomethines have
significant potential in sensing first row TM ions as these are
easy to synthesize in high purity and by changing the donor
atoms, the selectivity of the turn-on fluorescent probe may be
fine tuned towards specific transition metal ions.
Fig. 2 Visual changes in color after addition of aliquots of Fe(II) ion
to the podand (a) 2 and (b) 4.
Upon titration of Cr(III) ion with the podand 2, the intensity
of the peak at 388 nm decreased gradually; however, a new
peak at 274 nm appeared. Upon titration of 2 with Fe(II),
additionally, a new, low intensity, very broad peak at 650 nm
was observed with the peaks at B345 and 483 nm (as a left
shoulder in peak of 388 nm) which are responsible for the
colorimetric detection of Fe(II) (Fig. 1b). A visual change from
yellow to blue to green (Fig. 2a) was gradually observed upon
addition of increasing equivalents of Fe(II) ions. Thus,
compound 2 recognizes the Fe(II) ion colorimetrically, in
addition to the fluorescence response.
SP and SSZ are thankful to DST, India for Fast-Track
Research Grants. PBP is thankful to UGC, India for fellowship.
We thank Dr. Pradipta Purkayastha and Dr. Prasun K. Mandal
(IISER Kolkata) for helpful discissions.
Notes and references
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The higher wavelength peaks (B345, 483 and broad peak at
650 nm) are responsible for the colorimetric detection of Fe(II).
To explain the nature of the electronic transition in Fe(II)
complexes, we have carried out DFT calculations (at B3LYP/
6-31G*/sdd) on the model complex 5, where only one arm of
o-methylthiophenyl substituted azomethine on the 2-position
of fluorene was considered. Optimization of singlet (low-spin)
and quintet (high-spin) state structures of 5 at B3LYP/
6-31G*/sdd level of theory showed that the quintet state is
more stable by 15.8 kcal molÀ1 than that of the singlet state. In
line with our assumption on the conformational changes, the
azomethine planes are twisted at B781 from the planes of the
fluorene moiety in the optimized structure of high spin complex
5 (Fig. S27w). TD-DFT calculations at the same level of theory
showed that the higher wavelength transitions arise from the
charge transfer from the fluorene moiety to the metal bound
azomethine fragment (b spin) or only azomethine fragment
(a-spin) (Fig. S28 and S29 and Table S2w).
With podand 2, Cr(III) and Fe(II) showed >300 and 270-fold
enhancement in fluorescence intensity, respectively. Absorption
and emission spectra of 3 and 4 on addition of Cr(III) and
Fe(II) showed similar types of changes to that of podand 2.
Upon addition of Cr(III) and Fe(II), a 71- and 51-fold enhance-
ment in fluorescence intensity was observed for podand 3,
respectively, whereas, podand 4 showed a 14- and 5-fold
increase in fluorescence intensity, respectively. The overall
detection limit for metals of these podands is around 10 mM.
In conclusion, we have introduced here a new concept for
the design of fluorescent probes where fluorescence enhance-
ment can be achieved as a result of conformational changes
which suppress the non-radiative modes (IC and ISC) of
fluorescence quenching. The ligand 1 having O, N donors acts
as a ‘turn-on’ probe toward Cu(II) as well as to Cr(III) and
Fe(II). The podands 2–4 having S/Se, N donors behave as
a ‘turn-on’ two dimensional (colorimetric and fluorimetric)
selective fluorescent probe towards Cr(III) and Fe(II) where
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This journal is The Royal Society of Chemistry 2011