The conjugate
d polyelectrolyte PPESO3 features a poly(phenylene ethynylene) backbonesubstitute
d with anionic 3-sulfonatopropyloxy groups. PPESO3 is quenche
d very efficiently (
KSV > 10
6M
-1) by cationic energy transfer quenchers in an amplifie
d quenching process. In the present investigation,stea
dy-state an
d picosecon
d time-resolve
d fluorescence spectroscopy are use
d to examine amplifie
dquenching of PPESO3 by a series of cyanine
dyes via singlet-singlet energy transfer. The goal of thiswork is to un
derstan
d the mechanism of amplifie
d quenching an
d to characterize important parametersthat govern the amplification process. Stea
dy-state fluorescence quenching of PPESO3 by three cationicoxacarbocyanine
dyes in methanol solution shows that the quenching efficiency
does not correlate withthe Förster ra
dius compute
d from spectral overlap of the PPESO3 fluorescence with the cyanines'absorption. The quenching efficiency is controlle
d by the stability of the polymer-
dye association complex.When quenching stu
dies are carrie
d out in water where PPESO3 is aggregate
d, changes observe
d in theabsorption an
d fluorescence spectra of 1,1',3,3,3',3'-hexamethylin
dotricarbocyanine io
di
de (HMIDC) in
dicatethat the polymer templates the formation of a J-aggregate of the
dye. The fluorescence
dynamics in thePPESO3/HMIDC system were probe
d by time-resolve
d upconversion an
d the results show that PPESO3to HMIDC energy transfer occurs on two
distinctive time scales. At low HMIDC concentration, the
dynamicsare
dominate
d by an energy transfer pathway with a time scale faster than 4 ps. With increasing HMIDCconcentration, an energy pathway with a time scale of 0.1-1 ns is active. The prompt pathway (
![](/images/gifchars/tau.gif)
< 4 ps)is attribute
d to quenching of
delocalize
d PPESO3 excitons create
d near the HMIDC association site, whereasthe slow phase is attribute
d to intra- an
d interchain exciton
diffusion to the HMIDC.