Conspectus
Chiral functional materials with circularly polarized luminescence
(CPL) have risen rapidly in recent years because of their fascinating
characteristics and potential applications in various research fields.
CPL refers to the differential spontaneous emission of left (L)- and
right (R)-handed circularly polarized light upon photon or electron
excitation. Generally, an outstanding CPL-active material needs to
possess a high luminescence dissymmetry factor (g
lum) (defined as 2(I
L – I
R)/(I
L + I
R) where I is the emission
intensity), which is between −2 and +2. Although the exciting
development in CPL-active materials was achieved, the modulation of
CPL signs is still a challenge. For small organic systems, a relatively
small g
lum value, one of the key parameters
of CPL, limits their practical applications. Searching for efficient
approaches for amplifying g
lum is important.
Therefore, over the past decades, besides optimizing the structure
of small molecules, many other strategies to obtain efficient CPL-active
materials have been developed. For instance, self-assembly has been
well demonstrated as an effective approach to amplify the supramolecular
chirality as well as the g
lum values.
On the other hand, chiral liquid crystals (CLCs), which are capable
of selective reflection of left- and right-handed circularly polarized
light, also to serve as a host matrix for endowing guest emitters
with CPL activity and high g
lum values.
However, self-assembly focuses on modulating the conformation and
spatial arrangement of chiral emitters. And the CPL of a luminophore-doped
CLC matrix depends on the helix pitch and band gap positions. Lately,
novel photophysical approaches to modulate CPL signs have gradually
emerged.
In this Account, we discuss the recent progress of
excited-state-regulation
involved CPL-active materials. The emergence, amplification, and inversion
of CPL can be adjusted through regulation of the excited state of
chiral emitters. For example, Förster resonance energy transfer
(FRET) can amplify the g
lum values of
chiral energy acceptors in chiral supramolecular assemblies. By combining
the concepts of photon upconversion and CPL, high-energy upconverted
circularly polarized emission was achieved under excitation of low-energy
light, accompanied by an amplified g
lum. In addition, the organic systems with unpaired electrons, i.e.,
charge transfer (CT) system and open-shell π-radical, show favorable
CPL properties, which can be flexibly tuned with an applied magnetic
field. It should be noted that these photophysical process are associated
with the excited state of chiral emitters. So far, while the main
focus is on the regulation of the molecular and supramolecular nanostructures,
direct regulation of the excited state of the chiral system will serve
as a new platform to understand and regulate the CPL activity and
will be helpful to develop smart chiroptical materials.