Communications
DOI: 10.1002/anie.201002203
Luminescence Probes
Reversible Three-State Switching of Multicolor Fluorescence Emission
by Multiple Stimuli Modulated FRET Processes within
Thermoresponsive Polymeric Micelles**
Changhua Li, Yanxi Zhang, Jinming Hu, Jianjun Cheng,* and Shiyong Liu*
Energy transfer between light-absorbing donors and energy-
receiving acceptors occurs on the nanometer distance scale.[1]
One of the key issues in designing effective multichromo-
phore luminescent systems is the precise spatial arrangement
of the fluorophores. By learning from elegant systems existing
in nature, researchers have exploited a variety of artificial
nanostructures such as dendrimers,[2] nanoparticles,[3] (multi-
layered) thin films,[4] and supramolecular assemblies[5] to
achieve nanoscale control and accurate location of chromo-
phores, leading to the modulation of luminescence efficiency
through the enhancement or restriction of fluorescence
resonance energy transfer (FRET) processes. In view of the
microenvironment complexity in certain bio-applications
such as imaging, biosensing, and clinical diagnosis, it is
highly desirable to combine the concept of external stimuli-
triggered activation/deactivation of specific emitting fluoro-
phores to achieve higher temporal and spatial detection
resolution. Although there are a few examples of luminescent
polymeric assemblies and nanoparticles exhibiting two-state
switching of luminescence,[6] systems exhibiting both rever-
sible three-state on/off switching of the fluorescence emission
and stimuli-responsive tuning of the spatial distributions of
FRET donors and acceptors (FRET efficiency) has, to our
knowledge, not been accomplished.
cesses (Scheme 1). The FRET system consists of one type of
donor dye and two types of acceptor dyes, and fluorescence
emission of the latter two can be switched on and off by
changes in pH and light irradiation (UV/Vis), respectively.
Such multicolor luminescent polymeric assemblies can act as
sensitive ratiometric probes for pH and temperature. Most
importantly, the detection sensitivity can be further improved
at elevated temperatures because of the closer proximity
between FRET donors and acceptors resulting from the
thermoresponsive collapse of micelle coronas.
Three polymerizable fluorescent dyes, NBDAE, pH-
switchable rhodamine B based monomer (RhBAM; synthe-
sis: Scheme S1, NMR data: Figure S1 in the Supporting
Information), and photoswitchable SPMA, were synthe-
sized.[7] Amphiphilic diblock copolymer, P(St-co-NBDAE-
co-SPMA)20-b-P(NIPAM-co-RhBAM)60, bearing NBDAE
and SPMA moieties in the hydrophobic polystyrene (PS)
block and RhBAM moieties in the thermoresponsive poly(N-
isopropylacrylamide) (PNIPAM) block was synthesized by
sequential reversible addition–fragmentation transfer
(RAFT) polymerization (Scheme S2, Figures S2 and S3 in
the Supporting Information).[8] For comparison, a series of
PS-b-PNIPAM diblock copolymers with varying combina-
tions of NBDAE, SPMA, and RhBAM residues were also
synthesized. The molecular parameters of all diblock copoly-
mers used in this work are summarized in Table S1 in the
Supporting Information.
Herein we report the fabrication of amphiphilic and
thermoresponsive diblock-copolymer-based luminescent
micelles exhibiting three-state switchable multicolor fluores-
cence emission by external stimuli-modulated FRET pro-
In aqueous solution, P(St-co-NBDAE-co-SPMA)20-b-
P(NIPAM-co-RhBAM)60 self-assembles into spherical
micelles, as evidenced from AFM results (Figure S4 in the
Supporting Information), which consist of PS cores embedded
with NBDAE and SPMA dyes and thermoresponsive
PNIPAM coronas embedded with RhBAM dyes.[9] Surface
tensiometry measurements at 258C revealed a critical micelle
concentration (CMC) of 2.3 ꢀ 10ꢀ3 gLꢀ1 (Figure S5 in the
Supporting Information). The micellar solution at a concen-
tration of 1.0 gLꢀ1 exhibits thermo-induced aggregation
above 288C owing to the well-known lower critical solution
temperature (LCST) phase-transition behavior of PNIPAM
coronas (Figure S6 in the Supporting Information).[10]
Dynamic laser light scattering (LLS) analysis further revealed
intensity-average hydrodynamic diameters hDhi of 50 nm and
36 nm for the micellar solution at 258C and 358C, respectively
(Figure S7 in the Supporting Information). A comparison of
AFM and dynamic LLS analysis results indicated the
shrinkage of the thickness of the micellar coronas from
approximately 18 to 11 nm upon heating above the LCST of
PNIPAM coronas.
[*] C. Li, Y. Zhang, J. Hu, Prof. Dr. S. Liu
CAS Key Laboratory of Soft Matter Chemistry
Hefei National Laboratory for Physical Sciences at
Microscale Department of Polymer Science and Engineering
University of Science and Technology of China
Hefei, Anhui 230026 (China)
Fax: (+86)551-360-7348
E-mail: sliu@ustc.edu.cn
Prof. Dr. J. Cheng
Department of Materials and Engineering
University of Illinois at Urbana-Champaign
1304 West Green Street, Urbana, IL 61801 (USA)
Fax: (+1)217-333-2736
E-mail: jianjunc@illinois.edu
[**] The financial support of the National Natural Scientific Foundation
of China (NNSFC) Project (20874092) and the Specialized Research
Fund for the Doctoral Program of Higher Education (SRFDP) is
gratefully acknowledged.
Supporting information for this article is available on the WWW
5120
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2010, 49, 5120 –5124