multibubble sonoluminescence and sonochemistry of f-transition elements pflieger r., 1 virot m., 1...
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Multibubble sonoluminescence and sonochemistry of f-transition elements
Pflieger R.,1 Virot M.,1 Chave T.,1 Schneider J.,2 Nikitenko S.I.,1
1ICSM, Marcoule, France, 2MPI, Potsdam, Germany
Institute for Separation Chemistry of Marcoule (ICSM), Laboratory of Sonochemistry in Complex Fluids (www.icsm.fr)
August 13-16, 2012, Singapore
Fluorescence of uranyl ions
Uranyl ion UO22+ is a major chemical form of uranium in aqueous solutions
Absorption and emission spectra of UO22+ in 0.1M HClO4
at 25°C (used in analysis)
Why U and lanthanides (Tb)?
U is a principal element of nuclear industry
Ln are the important fission products and also they are widely used in industry (catalysis, optics, medical diagnostics, etc.)
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Multifrequency reactor for MBSL and sonochemistry
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In HClO4 UO22+ exhibits
extremely weak MBSL
MBSL of 0.1M UO22+ in HClO4 and in H3PO at 203 kHz, 10°C, Ar. The inset shows the emission
spectrum of 0.2M UO22+ in 0.2 M HClO4 after photoexcitation at λ = 427 nm.
In H3PO4 MBSL of UO22+ is much
stronger than that in HClO4
Strong effect of acid
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UO22+ SL intensity is strongly influenced by the ultrasonic frequency
The strongest intensity of UO22+ SL is observed at 203 kHz ultrasound
exhibiting the highest total SL (0.5M H3PO4, Ar)
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Ultrabright SL of UO22+ in H3PO4 can be seen by the unaided eye!
30 sec
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The difference between HClO4 and H3PO4 is attributed to UO22+
quenching
Intramolecular quenching with coordinated water: (UO2
2+)* + H2O → UO2+ + H+ + OH•
Intermolecular quenching :
(UO22+)* + H2O2 → UO2
+ + H+ + HO2•
UO2+ + OH• (HO2
•, H2O2) → UO22+
Quenching of UO22+ MBSL with 1•10-2 M
H2O2. 203 kHz, 86 W, 7.2•10-3 M UO22+ 0.5 M
H3PO4, 10°C, Ar.
Stable phosphate complexes UO2Hx(PO4)n+(2-3n+x) strongly decrease both
intra- and intermolecular quenching
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Effect of UO22+ concentration – an effective tool to elucidate the
mechanism of excitation
SL photons are totally absorbed by UO22+
(>10-4 M)
SonophotoluminescenceIn diluted solutions
Contribution of collisional mechanism in concentrated
solutions
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MBSL of Tb(III) in aqueous solutions
There is no SL of Tb(III) in diluted (<0.05 M) solutions
Tb(III) absorption
MBSL spectra of 0.1M TbCl3 in water (11°C, Ar)
Tb(III) emission
________________________f, kHz Pac, W QY, a.u.________________________20 24 0.40203 47 0.17607 41 0.10PL 0.08________________________
In solutions Tb(III) is excited mostly via collisional mechanismCollisional excitation is stronger at low-frequency?
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MBSL of Tb(III) at the extended solid-liquid interface
(Ce0.9Tb0.1)PO4 sintered pellet, water, 20 kHz, Ar, 10°C
Tb(III) at the interface is excited via sonophotoluminescence mechanism
Pellet
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CONCLUSIONS
MBSL of UO22+ is the first observation of SL for radioactive elements
MBSL of UO22+ and Tb(III) is extremely sensitive to ultrasonic frequency
and to the presence of complexing reagents.
Intramolecular and intermolecular quenching strongly influence the intensity of UO2
2+ and Tb(III) MBSL
The mechanism of UO22+ MBSL seems to vary with uranium concentration:
sonophotoluminescence dominates in diluted solutions, and collisional excitation would add its contribution at higher UO2
2+ concentration
MBSL of Tb(III) in solutions is triggered mostly by collisional mechanism and by sonophotoluminescence at the extended solid/liquid interface
==============================This work was supported by French ANR program (ANR-10-BLAN-0810) NEQSON
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