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2.2. Experimental method
scanning with Δλ = 0 would include RF signal and resonance light scat-
tering (RLS) signal. Fig. 1(b) showed that the two signals overlap with
each other in the range of 516–587 nm, which indicates that the emis-
sion signal contains RF and resonance light scattering. The experimental
results indicated that the RF signal of PRY was very strong while the RLS
signal was weak in 516–587 nm. The intensity values of the emission
light signal were measured at 558 and 516 nm, respectively, and were
showed in Fig. 1(b). Because the intensity of RLS becomes weak with
the increase of the wavelength in accordance with the Rayleigh scatter-
ing law, namely I∝1/λ4, λ = 558 nm I ≈ IRF = 5260, λ = 516 nm
I ≈ IRLS = 36 and IRS,558 ﹤ IRS,516. The intensity ratio of the two signals
at 558 nm was about 1000:7. So, when the RF is measured at 558 nm,
the effect of RLS was negligible. In addition, the RF spectra (Fig. 1(a))
of PRY displayed some characteristics of spiky, narrow, symmetrical
and slippery, which could eliminate the effect of other concomitant
fluorescence substances, including Sal2 and [UO22+-Sal2] complex, on
the RF signal of PRY. Therefore, the accuracy and selectivity of this ana-
lytical method would be effectively enhanced.
2.2.1. Double cloud point extraction
An aliquot (6.0 mL) of standard or sample solution containing uranyl
was pipetted into 10 mL scaled-glass test tubes with conical bottom.
Then, 2.0 mL of pH 5.5 Tris-HCl buffer solution was added to the tube
and mix well. A mixture of 0.40 mL of Sal1 ethanol solution (as coordi-
nation agent) and 1.0 mL of TX-114 aqueous solution (2.0% w/v) (as ex-
traction solvent) was injected rapidly into the solution. After gently
shaking and heating in a thermostatic bath at 68 °C for 15 min, a cloudy
solution which consisted of very fine droplets of TX-114 dispersed into
the aqueous sample was formed. The mixture was then centrifuged for
3 min at 3500 rpm after cooling in an ice bath for 5 min, causing the dis-
persed fine droplets of the extraction phase to settle down to the bot-
tom of the tube. The supernatant aqueous phase was discarded. The
sticky micellar phase was diluted to 0.40 mL with 0.0050 mol L−1
H2SO4 solution and heated once again at 68 °C for 15 min. The cloudy so-
lution is divided into two layers by centrifuging after cooling, and the
supernatant aqueous phase containing uranyl was detected by photo-
catalytic RF method. Because the amount of uranyl in 6 mL sample solu-
tion is measured after preconcentration by dCPE in a final volume of
0.4 mL, the solution is concentrated by a factor of 15.
3.2. The characteristics of PRY fluorescence resonance
The RF spectra of the reaction system were shown in Fig. 2. PRY itself
has very strong RF in the range of 516 to 587 nm with the maximum
wavelength located at 558 nm (curve 1). Sal2 or [UO22+-Sal2] had no
RF (curves 2 or 3), which shows that concomitant Sal2 or [UO22+-Sal2]
did not interfere with the RF signal of PRY. The RF of PRY was almost un-
changed after the addition of uranyl (curve 4). The RF of PRY was slight-
ly decreased (curve 5) after addition of the oxidizing agent KBrO3 to the
solution of PRY. Adding of Sal2 did not influence the reaction speed of
PRY and KBrO3 (curve 6). The RF of the system observably decreased
after adding the UO22+ to the solution of PRY-KBrO3 (curve 7) due to
the photo-catalytic action of UO22+. When Sal2 was added to the solu-
tion of PRY-KBrO3-UO22+, the more obvious decrease of the RF intensity
was observed (curve 8), which indicated that Sal2 could effectively en-
hance the photo-catalytic activity of UO22+. When the concentration of
Sal2 remains constant, compared with the reagent blank solution with-
out UO22+, the decrease value of RF intensity at 558 nm was proportional
to the concentration of UO22+ (curves 9–15). Based on this, a new photo-
catalytic RF method could be established for the determination of ultra-
trace uranium.
2.2.2. Procedure
Into a 25 mL colorimeter glass tube several solutions were added in
the following order: 2.0 mL of Tris-HCl buffer solution, 2.0 mL of KBrO3
solution, 2.0 mL of PRY solution, 0.40 mL of Sal2 ethanol solution and the
extraction from the uranyl calibration solution or samples solution by
dPCE. The mixture was diluted to 25 mL with redistilled water and be
shaken well. The mixture was placed in the circulating tap water to
keep in room temperature, and at strong visible-light irradiation for
15 min. The RF spectrum was obtained by synchronously scanning
with Δλ = 0 from 500 to 650 nm in a 1-cm quartz cell with slit widths
of 2.5 nm for excitation and 5 nm for emission. The intensity of RF was
measured at 558 nm. The decreased RF intensity of the reaction system
was represented as ΔF = F0 − F, here F and F0 were the RF intensities of
the reaction system with and without uranyl, respectively.
3. Results and discussion
3.1. The fluorescence spectral characteristics of PRY
3.3. The comparison of the absorption and RF spectra of the system
The fluorescence excitation, emission and RF spectra of PRY were
shown in Fig. 1(a). The maximum excitation and emission wavelengths
are located at 547 and 564 nm, respectively, and the excitation spectra is
overlapped with the emission spectra over a wide wavelength range be-
cause the Stokes shift is very small. The maximum overlap of the spectra
is located at 558 nm, which is equal to the RF peak.
A comparison of the absorption and RF spectra of the system are
shown in Fig. 3. Fig. 3 shows that both Sal2 and [UO22+-Sal2] have a
strong absorption band in the wavelength range of 305–355 nm. The
maximum absorption of Sal2 was located at 323 nm (curve 1). After
adding the UO22+, the absorption decreased, accompanying the blue
shift of the maximum absorption from 323 to 311 nm (curve 2). This
showed that UO22+ might react with Sal2 to form a complex compound
The three dimensional fluorescence spectrum of PRY was obtained
and showed in Fig. 1(b). The light signal obtained by synchronously
Fig. 1. (a) The RF fluorescence (1), emission (2), excitation (3) spectra of PRY. (b) The three dimensional fluorescence spectra.