© 2021 The Author(s). Published by the Royal Society of Chemistry Mater. Adv., 2021, 2, 2031–2035 | 2031
Cite this: Mater. Adv., 2021,
2, 2031
The performance of conjugated polymers
as emitters for triplet–triplet annihilation
upconversion†
Riley O’Shea,
ab
Can Gao,
c
Tze Cin Owyong,
ab
Jonathan M. White
b
and
Wallace W. H. Wong *
ab
A series of poly(phenylene–ethynylene) copolymers with various aryl spacer units were synthesized for use
as emitters in triplet–triplet annihilation upconversion. The upconversion performance of these conjugated
polymers was compared to that of well-known poly(phenylene–vinylene) polymers, MEH-PPV and super
yellow, in chloroform solution. The copolymer containing anthracene units outperformed both reference
polymers recording a maximum upconversion quantum yield of 0.18%.
Introduction
Triplet–triplet annihilation upconversion (TTA-UC), also known
as triplet fusion upconversion, is a photochemical process by
which two lower energy photons can be combined to produce
one photon of higher energy.
1
It sees use in raising the
efficiency of solar cells above their thermodynamic limit (the
Shockley–Queisser limit).
2,3
Two chromophores are required in a typical TTA-UC system –
a triplet sensitizer and an annihilator/emitter.
1
The triplet
sensitizer absorbs a photon promoting it to its singlet excited
state (Fig. 1a). Intersystem crossing (ISC) leads to the formation
of the triplet excited state on the sensitizer. This triplet exciton
can then be transferred to an emitter molecule via triplet energy
transfer (TET). As the triplet exciton population of emitters
builds, two triplet excitons can combine leading to triplet–triplet
annihilation (TTA) generating a higher energy singlet exciton.
This singlet exciton then undergoes radiative decay releasing a
photon that is higher in energy than the photon absorbed by the
sensitizer.
Transition metal complexes are most commonly used as triplet
sensitizers but metal chalcogenide quantum dots have also been
used.
4,5
As for the emitter component, polycyclic aromatic hydro-
carbon molecules have been widely investigated.
6–9
Much less
well-established is the use of conjugated polymers as emitters in
TTA-UC.
10–14
It was shown in theoretical models that the extended
conjugation of these materials leads to improved triplet exciton
diffusion which may assist in TTA-UC performance.
15
Measure-
ments of TTA-UC systems containing conjugated polymers
showed some promise but accurate comparison of TTA-UC
efficiency has not been reported.
14,16
In this study, the TTA-UC
Fig. 1 Jablonski diagram depicting the process involved for TTA-UC (a).
Structures of poly(phenylene–vinylene)s, MEH-PPV and super yellow, and
copolymers based on poly(phenylene–ethynylene) investigated as emitters
for TTA-UC (b).
a
ARC Centre of Excellence in Exciton Science, School of Chemistry, University of
Melbourne, Parkville, VIC 3010, Australia. E-mail: wwhwong@unimelb.edu.au
b
School of Chemistry, Bio21 Institute, University of Melbourne, Parkville, VIC 3010,
Australia
c
Beijing National Laboratory for Molecular Sciences, Key Laboratory of Organic
Solids, Institute of Chemistry, Chinese Academy of Sciences, Beijing, China
† Electronic supplementary information (ESI) available. CCDC 1992339. For ESI
and crystallographic data in CIF or other electronic format see DOI: 10.1039/
d1ma00068c
Received 27th January 2021,
Accepted 19th February 2021
DOI: 10.1039/d1ma00068c
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