posted on 2020-10-21, 14:32authored byTzu-Wei Tseng, Hao Yan, Tomonori Nakamura, Shun Omagari, Ji-Seon Kim, Martin Vacha
Poly(9,9-dioctylfluorene)
(PFO) is one of the most important conjugated
polymer materials, exhibiting outstanding photophysical and electrical
properties. PFO is also known for a diversity of morphological phases
determined by conformational states of the main chain. Our goal in
this work is to address some of the key questions on formation and
dynamics of one such conformation, the β-phase, by following
in real time the evolution of fluorescence spectra of single PFO chains.
The PFO is dispersed in a thin polystyrene film, and the spectra are
monitored during the process of solvent vapor annealing with toluene.
We confirm unambiguously that the PFO β-phase segments are formed
on a true single-chain level at room temperature in the solvent-softened
polystyrene. We further find that the formation of the β-phase
is a dynamic and reversible process occurring on the order of seconds,
leading to repeated spontaneous transitions between the glassy and
β-phase segments during the annealing. Comparison of PFO with
two largely different molecular weights (Mw) shows that chains with lower Mw form
the β-phase segments much faster. For the high Mw PFO chains, a detailed Franck–Condon analysis
of the β-phase spectra shows a large distribution of the Huang–Rhys
factor, S, and even dynamic changes of this factor
occurring on a single chain. Such dynamics are likely a manifestation
of changing coherence length of the exciton. Further, for the high Mw PFO chains we observe an additional conformational
state, a crystalline γ-phase. The γ-phase formation is
also a spontaneous reversible process in the solvent-softened matrix.
The phase can form from both the β-phase and the glassy phase,
and the formation requires high Mw to
enable intersegment interactions in a self-folded chain.