414
Z.J. Chen et al. / Dyes and Pigments 94 (2012) 410e415
Fig. 7. Color (a, left) and fluorescence (b, right) change of sensor AM-PDIs (from left to right: AM-PDIs only; AM-PDIs þ Fꢂ; AM-PDIs þ Clꢂ; AM-PDIs þ Brꢂ; AM-PDIs þ Iꢂ).
stretching vibrational absorption(3294.93 cmꢂ1
)
disappeared
selective for fluoride anions over other halid ions. The large red
shift in the absorption and the ratiometric fluorescent response
render the sensor suitable for detection of F anions by simple
visual inspection.
with addition of Fꢂ, which confirmed the deprotonation of NeH
by Fꢂ.
Fig. 4a showed a nearelinear correlation of AM-PDIs between
intensity ratios of absorbance at 681 nm to those at 530 nm (A681
/
A530) vs fluoride ion concentration in DCM.This demonstrated the
potential utility of sensor AM-PDIs for calibrating and determining
fluoride ion concentration in DCM. Furthermore, a corresponding
correlation between emission ratiometric response of AM-PDIs at
580 nm and 488 nm (I488/I580) and fluoride ion concentration in
DCM was obtained in Fig. 4b, thus, AM-PDIs could also serve as
a ratiometric fluorescent sensor for Fꢂ. The linear equation was
found to be y ¼ 533.22 ꢁ 105x þ 25.309 (R ¼ 0.9652), where y was
the absorbance at 681 nm measured at a given F1 concentration
and x represented the concentration (10ꢂ5 mol/L) of F added.
According to IUPAC, the detection limit was determined from
three times the standard deviation of the blank signal (3s) as
Acknowledgements
This research was financially supported by the National Nature
Science Foundation of China (20672035) and Baihehua Group.
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4. Conclusions
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limit was calculated to be 0.14 mM. In addition, the sensor is highly