Study on the radiative D-5(4) -> F-7(j) relaxation dynamics of Tb(III) in electrochemically excited self-assembled dimeric heterodinuclear Tb(III)-Ln(III)' chelates
T. Ala-kleme et al., Study on the radiative D-5(4) -> F-7(j) relaxation dynamics of Tb(III) in electrochemically excited self-assembled dimeric heterodinuclear Tb(III)-Ln(III)' chelates, ANALYT CHIM, 403(1-2), 2000, pp. 161-171
A study has been conducted to explore the inter-lanthanide(III) energy inte
ractions in self-assembled dimeric heterodinuclear 1-Tb(III)-Ln(III)'-1 che
lates (Ln(III)' = Dy(III), Nd(III), Y(III), Yb(III)) (1 = 2,6-bis[N,N-bis (
carboxymethyl) -aminomethyl]4-benzoylphenol]) and their effects on the elec
trochemically initiated radiative D-5(4) --> F-7(j) transitions of Tb(III)
of these dinuclear chelates at a cathodically pulse-polarized oxide-covered
aluminium electrode. From the selected heterodinuclear Tb(III)-Ln(III)' ed
ifices, (i) the Tb(III)-Dy(III) edifice initiates the exceptionally shea-li
ved D-5(4) --> F-7(j) transitions of Tb(III) with k(i) approximate to 9.0 m
s(-1) mainly due to the competitive inter-lanthanide(III) Tb(III)-Dy(III) D
-5(4) --> F-4(9/2) back energy transfer, (ii) likewise, the Tb(III)-Y(III)
edifice initiates the D-5(4) --> F-7(j) transitions of Tb(III) with k(i) ap
proximate to 1.4 ms(-1) caused by the absence of any Y(III)-specific energy
level capable of acting as the acceptor level for the ligand-specific (3)p
i pi* and/or Tb(III)-specific D-5(4) relaxations and, finally, (iii) the Tb
(III)-Nd(III) and Tb(III)-Yb(III) edifices do not generate these radiative
Tb(III) specific transitions; in the case of Ln(III)' = Nd(III), this inhib
ition originates from the preferential ligand-specific 3 pi pi* relaxation
to the Nd(III)-specific acceptor levels while in the case of Ln(III)' = Yb(
III), this 3 pi pi* relaxation seems to occur directly to the excited F-2(5
/2) state of Yb(III) by the ET intermediate. (C) 2000 Elsevier Science B.V.
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