Yining Tao1,2, Chenxu Yan2, Dan Li2, Jianfeng Dai2, Yingsheng Cheng1, Hui Li1, Wei-Hong Zhu2, Zhiqian Guo2. 1. Department of Interventional Radiology, Shanghai Jiao Tong University Affiliated Sixth People's Hospital, Shanghai 200233, China. 2. Key Laboratory for Advanced Materials and Joint International Research Laboratory of Precision Chemistry and Molecular Engineering, Frontiers Science Center for Materiobiology and Dynamic Chemistry, Shanghai Frontiers Science Center of Optogenetic Techniques for Cell Metabolism, Institute of Fine Chemicals, School of Chemistry and Molecular Engineering, East China University of Science and Technology, Shanghai 200237, China.
Abstract
Pancreatic ductal adenocarcinoma (PDAC), as one of the most malignant tumors with dense desmoplastic stroma, forms a specific matrix barrier to hinder effective diagnosis and therapy. To date, a paramount challenge is in the search for intelligent nanotheranostics for such hypopermeable tumors, especially in breaking the PDAC-specific physical barrier. The unpredictable in vivo behaviors of nanotheranostics, that is, real-time tracking where, when, and how they cross the physical barriers and are taken up by tumor cells, are the major bottleneck. Herein, we elaborately design sequence-activated nanotheranostic TCM-U11&Cy@P with dual-channel near-infrared fluorescence outputs for monitoring in vivo behaviors in a sequential fashion. This nanotheranostic with a programmable targeting capability effectively breaks through the PDAC barriers. Ultimately, the released aggregation-induced emission (AIE) particle TCM-U11 directly interacts with PDAC cells and penetrates into the deep tissue. Impressively, this fluorescent nanotheranostic intraoperatively can map human clinical PDAC specimens with high resolution. We believe that this unique sequence-activated fluorescent strategy expands the repertoire of nanotheranostics in the treatment of hypopermeable tumors.
Pancreatic ductal adenocarcinoma (PDAC), as one of the most malignant tumors with dense desmoplastic stroma, forms a specific matrix barrier to hinder effective diagnosis and therapy. To date, a paramount challenge is in the search for intelligent nanotheranostics for such hypopermeable tumors, especially in breaking the PDAC-specific physical barrier. The unpredictable in vivo behaviors of nanotheranostics, that is, real-time tracking where, when, and how they cross the physical barriers and are taken up by tumor cells, are the major bottleneck. Herein, we elaborately design sequence-activated nanotheranostic TCM-U11&Cy@P with dual-channel near-infrared fluorescence outputs for monitoring in vivo behaviors in a sequential fashion. This nanotheranostic with a programmable targeting capability effectively breaks through the PDAC barriers. Ultimately, the released aggregation-induced emission (AIE) particle TCM-U11 directly interacts with PDAC cells and penetrates into the deep tissue. Impressively, this fluorescent nanotheranostic intraoperatively can map human clinical PDAC specimens with high resolution. We believe that this unique sequence-activated fluorescent strategy expands the repertoire of nanotheranostics in the treatment of hypopermeable tumors.
Poorly permeable tumors,
with the unique stroma-rich microenvironment,
severely limit the site-specific bioavailability of nanotheranostics,
preventing the achievement of clinical efficacy.[1−4] For example, pancreatic ductal
adenocarcinoma (PDAC) is an extremely malignant tumor with a high
fatality rate and reported an overall five-year survival rate of less
than 10%.[5,6] Unfortunately, PDAC is extremely difficult
to diagnose due to its hidden location, lack of specific symptoms,
and aggressive behavior.[7,8] Most current strategies
for incremental improvements to such solid tumors merely rely on the
enhanced permeability and retention (EPR) effect or active targeting
ligands.[9−11] However, the natural protective physical barrier
from a dense desmoplastic stroma becomes a major obstacle for the
effective diagnosis and treatment of PDAC, thereby hindering deep
and uniform penetration of nanotheranostics.[12−14] Even with the
incorporation of active targeting moieties, cellular uptake in PDAC
deep tissues still faces the substantial barrier of nanoparticle internalization
only within the first few layers of tumor cells (proximal to the vasculature).[15−17] To date, a paramount challenge is in the search for intelligent
nanotheranostics for such hypopermeable tumors, especially in breaking
the PDAC-specific physical barrier.Toward this goal, the programmable-responsive
strategy that tunes
their properties (e.g., regulating particle size, exposing active
targeting ligand, etc.)[18−22] in response to environmental stimuli would realize robust and effective
delivery to deep PDAC tissue.[23−25] In particular, it is still a
critical challenge to reveal the in vivo behavior
of these nanotheranostics, that is, real-time tracking where, when,
and how they cross the PDAC barriers and are taken up by tumor cells.
For instance, the size of nanoparticles could be tailored for purposes
of improving tumor permeability for PDAC, but still little is known
about the real-time pathways in which the stimuli-induced particle
change occurs.[26−28] Specifically, toward breaking the PDAC-specific matrix
barrier, such nanotheranostics require monitoring multistaged in vivo behaviors in a sequential fashion and synergistically in situ initiating intratumoral therapy. Inspired by the
Boolean logic idea,[29−32] we envisioned that the integration of interactional fluorophores
with activatable dual-emission into nanotheranostics is the key strategy
to solve this dilemma, which would greatly expand the repertoire of
programmable-responsive nanotheranostics in the treatment of hypopermeable
tumors.Herein, we innovatively present a programmable targeting
strategy
of sequence-activated fluorescent nanotheranostics for effectively
crossing the PDAC-specific matrix barrier, wherein all of these sequential in vivo behaviors are monitored via activatable dual-channel
near-infrared (NIR) fluorescence to enhance tumor permeability and
therapeutic efficacy. As illustrated in Figure , this fluorescent nanotheranostic (named
TCM-U11&Cy@P) contains three components: the diblock copolymer
serving as the carrier with ultrasensitive response to pH, AIEgen
TCM-DN (FRET donor) covalently attached with U11 peptide (TCM-U11)
for targeting PDAC cells, and the cyanine fluorophore (Cy) as an NIR
Förster resonance energy transfer (FRET) acceptor. First of
all, TCM-U11&Cy@P remains nonemissive and maintains a relatively
large particle size at the normal pH of 7.4. After being delivered
reaching the tumor site through passive tumor targeting (EPR effect),
TCM-U11&Cy@P dissociates under pH <6.8, along with the release
of the Cy (fluorescence enhancement at 830 nm) and small AIEgen nanoparticles
(size <50 nm). Owing to the pH-triggered size transformation by
the acidic tumor microenvironment, the resulting small AIE nanoparticles
could further penetrate into the deep PDAC tissue, and thus, the fluorescence
enhancement at 650 nm could real-time monitor the pathways in which
the stimuli-induced particle size change occurs. Then, the surface-grafted
U11 peptides of AIE nanoparticles are directly exposed and thereby
bind to receptors (uPAR) overexpressed on PDAC cells, markedly facilitating
cellular internalization and remarkable reactive oxygen species generation
for photodynamic therapy (PDT) in living mice. Notably, this programmable
targeting strategy offers unique capabilities in dual-channel monitoring in vivo physiological processes, thereby making a breakthrough
of inherent PDAC-specific physical barriers. Notably, the efficiently
enhanced intratumoral distribution of this nanotheranostic allows
for intraoperatively mapping clinical specimens with high resolution.
This unique sequence-activated fluorescent nanotheranostic would pave
a promising avenue toward reporting specific targeting imaging and
an effective therapeutic process for universal poorly permeable tumors.
Figure 1
Schematic
illustration of sequence-activated fluorescent nanotheranostics
for programmable targeting of the pancreatic tumor. (i) Owing to the
passive tumor targeting, TCM-U11&Cy@P with an initially large
particle size is delivered to tumor tissue via the enhanced penetration
and retention (EPR) effect. (ii) In an acidic tumor microenvironment,
TCM-U11&Cy@P executes micelle dissociation, followed by the release
of the Cy (emission at 830 nm) and TCM-U11 particles (broad emission
at 650 nm). Owing to this tumor microenvironment-triggered size transformation,
the resulting small AIE particles could be further delivered into
the deep PDAC tissue, and the fluorescence enhancement at 650 nm could
track the pathways in which the stimuli-induced particle change occurs.
(iii) Then, the surface-grafted U11 peptides of TCM-U11 particles
target to the receptors (uPAR) overexpressed on PDAC cells in the
deep tissue and thereby facilitate deep PDT to ablate the tumor.
Schematic
illustration of sequence-activated fluorescent nanotheranostics
for programmable targeting of the pancreatic tumor. (i) Owing to the
passive tumor targeting, TCM-U11&Cy@P with an initially large
particle size is delivered to tumor tissue via the enhanced penetration
and retention (EPR) effect. (ii) In an acidic tumor microenvironment,
TCM-U11&Cy@P executes micelle dissociation, followed by the release
of the Cy (emission at 830 nm) and TCM-U11 particles (broad emission
at 650 nm). Owing to this tumor microenvironment-triggered size transformation,
the resulting small AIE particles could be further delivered into
the deep PDAC tissue, and the fluorescence enhancement at 650 nm could
track the pathways in which the stimuli-induced particle change occurs.
(iii) Then, the surface-grafted U11 peptides of TCM-U11 particles
target to the receptors (uPAR) overexpressed on PDAC cells in the
deep tissue and thereby facilitate deep PDT to ablate the tumor.
Results and Discussion
Constructing Sequence-Activated
Nanotheranostics
As
mentioned above, PDAC is the most stroma-rich tumor in all solid tumors,
and its dense desmoplastic stroma makes it difficult to achieve a
better performance by passive targeting or active targeting.[33−35] That is, the current “single-locked” nanotheranostics
are unable to alter their targeting properties in the specific intratumoral
region, which inevitably limits their tumor distribution. In this
case, it is urgent to develop a sequence-activated targeting strategy
to break the barrier characterized by low vascularity and dense fibrosis
for improving the tumor targeting efficiency of PDAC.Toward
this programmable in vivo targeting strategy, peptide-based
ligands could be primarily considered as an active targeting unit.
Herein, to enhance the specific uptake efficiency of PDAC cells, U11
peptide was chosen due to its high affinity to the PDAC-cell receptors
(uPAR).[36−38] In this case, we covalently attached U11 peptides
to NIR AIEgen (TCM-DN, emission at 650 nm) to form small AIE nanoparticles
with surface-grafted U11 peptides (TCM-U11; Figure ).[39−43] Subsequently, we chose a diblock copolymer (named PolypH) as a pH-activated nanocarrier, which is composed of a PEG unit
and copolymerized hexamethyleneimino-functionalized methacrylate.[44−47] Importantly, this block copolymer PolypH not only maintains
the TCM-U11 inside the nanoparticles in normal tissues but also promises
the efficient release of TCM-U11 at the acidic tumor site.Aiming
toward real-time tracking the delivery, distribution, and
release of TCM-U11 to PDAC cells without a blind spot, we described
a dual-channel NIR fluorescence strategy, that is, TCM-U11 and another
NIR indicator Cy (emission at 830 nm) which were coloaded into the
PolypH matrix. Specifically, the dissolved mixture of TCM-U11,
Cy, and PolypH into DMSO was added dropwise into the ultrapure
water. Then, the DMSO and unloaded agents were removed via dialysis
to obtain uniform TCM-U11&Cy@P nanoparticles. All of the detailed
synthetic routes and characterization of TCM-U11, Cy, and PolypH are depicted in the Supporting Information, and the high-resolution mass spectrometry and 1H NMR
measurements were made to fully characterize the peptide-decorated
TCM-U11 (Figures S1–S4 in the Supporting
Information). Besides, as the controls, we also constructed Cy@P,
TCM@P (only TCM-DN loaded), and TCM-U11@P (only TCM-U11 loaded, Figure S5 in the Supporting Information). From
the dynamic light scattering (DLS) test, TCM-U11&Cy@P displayed
a uniform size of 107 nm (Table S1 in the
Supporting Information). Notably, the TCM-U11&Cy@P nanoparticles
displayed a uniform size within 72 h, suggesting their excellent stability
(Figure S6 in the Supporting Information).
The ζ potential value of TCM-U11&Cy@P was 17.8 mV. Moreover,
the CMC value was calculated to be only about 0.84 mgmL–1, confirming the compact and stable nanostructure of TCM-U11&Cy@P
(Figure S7 in the Supporting Information).
All of these results indicated that our elaborately designed TCM-U11&Cy@P
possessed well-controlled, uniform, and stable nanostructures.
Revealing
Long-Wavelength AIE Characteristics of TCM-DN
High-fidelity
imaging and efficient treatment are of great importance
for the PDAC theranostic.[48−52] With this in mind, we chose TCM as the building block for endowing
AIEgens with bright NIR emission and excellent photosensitive properties.[53] By introducing electron-donating carbazol and
a π-bridge (thiophene unit) into the TCM unit, we obtained the
long-wavelength AIEgen TCM-DN. Next, the AIE and PDT characteristics
of TCM-DN were investigated (Figure ). Owing to its hydrophobicity, TCM-DN was highly soluble
in DMSO but became an aggregated state in water. With the increasing fw from 0% to 90%, the fluorescence intensity
significantly increased, accompanied by an obvious red shift in emission.
In particular, TCM-DN showed strong fluorescence in the mixed fw = 80% DMSO/water solution in contrast with
that in pure DMSO solution, which further confirmed its typical AIE
property (Figure a,b).
Furthermore, to evaluate the reactive oxygen species (ROS) generation
capability of TCM-DN, 9,10-anthracenediyl-bis(methylene)-dimalonic
acid (ABDA) was utilized as the ROS indicator by the oxidation-induced
decrease of absorbance.[54−59] Upon light irradiation with TCM-DN aggregates, the absorption peak
of ABDA sharply decreased, confirming the highly efficient production
of ROS of TCM-DN (Figure c,d). In addition, the time-dependent absorbance of TCM-DN
upon continuous illumination demonstrated that it had a 92-fold longer
half-life time (∼1200 s) than ICG (∼13 s, FDA-approved
NIR contrast agent). Obviously, TCM-DN exhibited a much better photostability
than ICG, demonstrating its great benefit for bioimaging (Figure S8 in the Supporting Information). Moreover,
TCM-DN nanoaggregates displayed excellent stability in different pH
values (Figure S9 in the Supporting Information).
Taken together, our designed TCM-DN showed high-performance AIE and
photosensitive properties, indicating its potential capability in
high-fidelity bioimaging.
Figure 2
Spectral properties of the significant AIE performance
and photodynamic
effect of TCM-DN. (a) Fluorescence emission spectra of TCM-DN (10–5 M) in DMSO/water mixtures with different volume fractions
of water (fw), λex =
510 nm. (b) I/I0 plots
of TCM-DN in a mixture of DMSO/water, where I is
the fluorescence intensity at 650 nm, and I0 is the fluorescence intensity of TCM-DN in 80% water, λex = 510 nm. Inset: fluorescent photoimages in pure DMSO solvent
and DMSO/water solution of TCM-DN under light illumination. (c) UV–vis
absorption spectra of ABDA in the presence of TCM-DN under light irradiation
(0.10 W cm–2, 4 min, 400–700 nm). (d) Normalized
absorbance intensity of ABDA at 380 nm after photodecomposition by
ROS upon light irradiation.
Spectral properties of the significant AIE performance
and photodynamic
effect of TCM-DN. (a) Fluorescence emission spectra of TCM-DN (10–5 M) in DMSO/water mixtures with different volume fractions
of water (fw), λex =
510 nm. (b) I/I0 plots
of TCM-DN in a mixture of DMSO/water, where I is
the fluorescence intensity at 650 nm, and I0 is the fluorescence intensity of TCM-DN in 80% water, λex = 510 nm. Inset: fluorescent photoimages in pure DMSO solvent
and DMSO/water solution of TCM-DN under light illumination. (c) UV–vis
absorption spectra of ABDA in the presence of TCM-DN under light irradiation
(0.10 W cm–2, 4 min, 400–700 nm). (d) Normalized
absorbance intensity of ABDA at 380 nm after photodecomposition by
ROS upon light irradiation.
Tracking Sequence-Activated pH-Triggered and Size Transformation
Process via Dual-Channel Fluorescence
As is known, most stimuli-responsive
nanoparticles suffer from only one “always-ON” readout
channel, which makes them unable to understand multistaged behavior
in a certain tumor microenvironment in real time.[60−62] In this case,
we hypothesized that the Förster resonance energy transfer
(FRET) strategy could make a breakthrough for achieving AIE-active
responses and thereby implement a real-time monitoring sequence-activated
trigger process (Figure a and Figure S10 in the Supporting Information).[63−65] In this case, the coloaded longer-wavelength NIR fluorophore Cy
(cyanine) was chosen as the quencher (FRET acceptor) of the “always-ON”
AIEgen TCM-DN (FRET donor). To confirm the feasibility of this FRET-induced
AIE quenching, we then investigated the absorption/fluorescence spectral
properties of TCM-DN and Cy units. As expected in Figure b and Figure S11 in the Supporting Information, there was a significant
spectral overlap between the fluorescence spectrum of TCM-DN and the
absorption spectrum of Cy, implying the possibility of a FRET effect
from TCM-DN to the Cy moiety.
Figure 3
FRET-induced dual-channel response for tracking
the sequence-activated
process. (a) As is well-known, relatively large nanoparticles (size
>50 nm) with the assistance of the EPR effect possess superior
tumor
accumulation, while relatively small nanoparticles (size <50 nm)
could undergo minimal adhesion to the extracellular matrix for improving
tumor penetration. Hence, the trade-off effect between tumor accumulation
and deep delivery requires a fine regulation of the size and morphology
of nanoparticles for sufficient penetration. In our design, the nanotheranostic
TCM-U11&Cy@P can disassemble in the acidic tumor microenvironment,
alone with the dual-channel response and size transformation. (b)
Fluorescence spectra (λex = 510 nm, 37 °C) of
TCM-DN and excitation spectra (λex = 730 nm, 37 °C)
of Cy in water/DMSO (fw = 50 vol %). Fluorescence
spectra of TCM-U11&Cy@P in aqueous solution at pH 7.0 and 6.0
at λex = 510 nm (c) and λex = 730
nm (d). Fluorescence intensity as a function of pH for TCM-U11&Cy@P
at 830 nm (e) and 650 nm (f). The nanoprobe displays a sharp pH response
(pKa = 6.8, ΔpHON/OFF = 0.3). At pH > pKa (6.8), the nanoprobe
self-assembles as a compact micelle, leading to fluorescence quenching
at both 650 and 830 nm. At pH < pKa (6.8), the nanoprobe can be activated (micelle disassembly) and
emits bright fluorescent signals at both 650 and 830 nm. (g) Hydrodynamic
diameters of TCM-U11&Cy@P at pH 7.4 and 6.5 in aqueous solution.
FRET-induced dual-channel response for tracking
the sequence-activated
process. (a) As is well-known, relatively large nanoparticles (size
>50 nm) with the assistance of the EPR effect possess superior
tumor
accumulation, while relatively small nanoparticles (size <50 nm)
could undergo minimal adhesion to the extracellular matrix for improving
tumor penetration. Hence, the trade-off effect between tumor accumulation
and deep delivery requires a fine regulation of the size and morphology
of nanoparticles for sufficient penetration. In our design, the nanotheranostic
TCM-U11&Cy@P can disassemble in the acidic tumor microenvironment,
alone with the dual-channel response and size transformation. (b)
Fluorescence spectra (λex = 510 nm, 37 °C) of
TCM-DN and excitation spectra (λex = 730 nm, 37 °C)
of Cy in water/DMSO (fw = 50 vol %). Fluorescence
spectra of TCM-U11&Cy@P in aqueous solution at pH 7.0 and 6.0
at λex = 510 nm (c) and λex = 730
nm (d). Fluorescence intensity as a function of pH for TCM-U11&Cy@P
at 830 nm (e) and 650 nm (f). The nanoprobe displays a sharp pH response
(pKa = 6.8, ΔpHON/OFF = 0.3). At pH > pKa (6.8), the nanoprobe
self-assembles as a compact micelle, leading to fluorescence quenching
at both 650 and 830 nm. At pH < pKa (6.8), the nanoprobe can be activated (micelle disassembly) and
emits bright fluorescent signals at both 650 and 830 nm. (g) Hydrodynamic
diameters of TCM-U11&Cy@P at pH 7.4 and 6.5 in aqueous solution.Encouraged by the aforementioned obvious spectral
overlap, we then
studied the FRET-induced dual-channel fluorescence responses of TCM-U11&Cy@P
with pH change. At pH 7.0, TCM-U11&Cy@P showed nonfluorescence
neither at 830 nm (from Cy) nor at 650 nm (from TCM-U11) (Figure c,d). This dual emission
complete quenching between the two fluorophores could be attributed
to the following: (i) TCM-U11&Cy@P formed a compact self-assembled
micelle at pH 7.4, leading to the typical aggregation-caused quenching
(ACQ) property of Cy in its compact state. (ii) Owing to the FRET
effect between TCM-DN and the Cy unit, the fluorescence of TCM-DN
was also effectively quenched from an intermolecular energy transfer.[66,67] Thus, we successfully obtained the AIE fluorescence quenching signal
based on the FRET strategy. Given that a pH-response nanocarrier was
employed in this nanotheranostic, we reasoned that the change in pH
could remarkably influence the efficiency of the FRET process and
result in dual-channel fluorescence.To verify the possibility
of the pH-triggered dual-channel fluorescence
changes, we further investigated the spectral properties of TCM-U11&Cy@P
under acidic conditions. When the pH was decreased to 6.0, the protonation
of the hydrophobic block caused the disassembly of the initial compact
micelle, leading to a dramatic NIR fluorescence signal enhancement
at both 830 and 650 nm (Figure c,d). Specifically, the fluorescence intensities at 830 nm
(from Cy) and 650 nm (from TCM-U11) were amplified over 80-fold and
8-fold, respectively. Also, the TCM-U11&Cy@P nanoparticles showed
an extremely sharp pH response (ΔpHON/OFF = 0.3)
at pH 6.8 (Figure e,f). This significant fluorescence enhancement could be attributed
to the following: (i) TCM-U11&Cy@P dissociated in the acidic condition
with the release of cyanine dyes, leading to the fluorescence recovery
at 830 nm. (ii) TCM-U11 was also released and formed small AIE nanoparticles.[68,69] Consequently, the donor–acceptor distance was beyond the
operating range of FRET, resulting in the enhancement of TCM-U11 at
650 nm. All of these results strongly supported the fact that the
proposed sequence-activated nanotheranostic TCM-U11&Cy@P had the
desired capacity for real-time tracking of the programmed acidic pH-triggered
and subsequent size transformation process via dual-channel fluorescence.To validate the concomitant size responses with the turn-on NIR
emission signals at both 830 and 650 nm, we further studied the acidic
pH-triggered size response of TCM-U11&Cy@P by transmission electron
microscopy (TEM) and dynamic light scattering (DLS). As shown in Figure g and Figure S12 in the Supporting Information, with
the decreasing of pH value, TCM-U11&Cy@P displayed an obvious
size change from 68 to 12 nm, indicating the dissociation of the initial
nanoparticles. Also, this acidic-triggered size reduction was consistent
with the dual-channel fluorescence responses (Figure c–f). Consequently, the size transformable
functionality was expected to break the trade-off effect between tumor
accumulation and deep delivery required in pancreatic cancer theranostics.
Most importantly, the FRET-induced dual-channel fluorescence changes
successfully finely regulated the AIE-active signal and thereby made
it possible to track the sequence-activated process with high fidelity.
Targeting Pancreatic Cancer Cell with High-Fidelity Imaging
As is well-known, compared with small molecules, nanoparticles
could improve intracellular retention and achieve long-time tracking
of living cells.[70−74] We thus hypothesized that our designed TCM-U11&Cy@P that combines
a well-defined nanostructure and programmable targeting could further
promote cellular internalization and imaging performance toward pancreatic
cancer cells (PANC-1 cells). In order to evaluate the PANC-1 cell-specific
imaging of TCM-U11&Cy@P, we also utilized TCM-DN, TCM-U11, TCM@P
(only TCM-DN loaded), and TCM-U11@P (only TCM-U11 loaded) as the controls
(Figure S5 in the Supporting Information).As shown in Figure a,b, compared with TCM-DN, TCM-U11 displayed a brighter fluorescence
signal in PANC-1 cells, which strongly confirmed the active targeting
ability of the U11 peptide. Furthermore, it was found that TCM@P showed
a much brighter fluorescence signal than TCM-DN, indicating that the
well-defined nanostructure could improve the cell uptake efficiency
(Figure c and Figure S13 in the Supporting Information). Importantly,
TCM-U11@P displayed the brightest AIE fluorescence signal among TCM-DN,
TCM-U11, and TCM@P. It was implied that the well-defined nanostructure
with a U11 peptide-mediated active targeting ability could execute
highly specific PANC-1 cell binding (Figure d,f). In TCM-U11&Cy@P, bright NIR signals
at both 830 and 650 nm were observed in Figure e and Figure S13 in the Supporting Information. In conjunction with the dual-channel
imaging results, it could be concluded that we successfully developed
a sequence-activated logic nanoprobe for the selective sensing and
targeting of PANC-1 cells.
Figure 4
Dual-channel fluorescence for tracking the excellent
targeting
capability to PANC-1 cells. (a–e) Dual-channel confocal images
of PANC-1 cells incubated with TCM-DN, TCM-U11, TCM@P, TCM-U11@P,
and TCM-U11&Cy@P. Note: The green channel (λex = 730 nm, λem = 830 nm) indicates the fluorescence
from Cy, and the red channel (λex = 510 nm, λem = 650 nm) indicates the fluorescence from TCM-DN. (f) Relative
cellular fluorescence intensity under treatment with groups of nanoprobes.
Note: Fluorescence images of cells were analyzed by ImageJ software.
The experiment is performed three times independently. Data with error
bars are expressed as mean ± s.d., n = 3 biologically
independent cells. The P value was calculated by
the Student’s t test. ***p < 0.001. (g) Western blot results of uPAR levels between normal
MS1 cells and PANC-1 cells. (h) Quantitative analysis of uPAR levels
from a Western blot assay. The experiment is performed three times
independently, and GAPDH is used as a loading control. ***p < 0.001. (i–l) Flow cytometry analysis of cellular
uptake of TCM-DN, TCM-U11, TCM@P, and TCM-U11@P in PANC-1 cells.
Dual-channel fluorescence for tracking the excellent
targeting
capability to PANC-1 cells. (a–e) Dual-channel confocal images
of PANC-1 cells incubated with TCM-DN, TCM-U11, TCM@P, TCM-U11@P,
and TCM-U11&Cy@P. Note: The green channel (λex = 730 nm, λem = 830 nm) indicates the fluorescence
from Cy, and the red channel (λex = 510 nm, λem = 650 nm) indicates the fluorescence from TCM-DN. (f) Relative
cellular fluorescence intensity under treatment with groups of nanoprobes.
Note: Fluorescence images of cells were analyzed by ImageJ software.
The experiment is performed three times independently. Data with error
bars are expressed as mean ± s.d., n = 3 biologically
independent cells. The P value was calculated by
the Student’s t test. ***p < 0.001. (g) Western blot results of uPAR levels between normal
MS1 cells and PANC-1 cells. (h) Quantitative analysis of uPAR levels
from a Western blot assay. The experiment is performed three times
independently, and GAPDH is used as a loading control. ***p < 0.001. (i–l) Flow cytometry analysis of cellular
uptake of TCM-DN, TCM-U11, TCM@P, and TCM-U11@P in PANC-1 cells.To verify the U11 peptide targeting to the receptors
(uPAR) overexpressed
on PANC-1 cells, the uPAR levels between normal cells (MS1 cells)
and PANC-1 cells were determined by Western blot assays.[75,76] As expected, these results showed the overexpression of uPAR in
PANC-1 cells, which was much higher than that of normal cells (Figure g,h). Thus, the active
targeting of the U11 peptide toward uPAR was effective, confirming
the active targeting ability of TCM-U11&Cy@P. All f the cell imaging
and Western blot assays demonstrated that the programmable targeting
strategy significantly improved the specific targeting ability toward
PANC-1 cells.To quantitatively evaluate the internalization
of TCM-U11&Cy@P
by PANC-1 cells, the properties of nanoparticles were further analyzed
by flow cytometry.[77] First, we evaluated
the effect of incubation time on the uptake of PANC-1 cells. As illustrated
in Figure i, it took
18 h for the cellular uptake ratios of TCM-DN to increase from 0.2%
to only 3.2%. Subsequently, we observed the slower uptake ratios of
TCM-U11 (7.9%, Figure j). In contrast, within only 3 h, the uptake ratios of TCM@P and
TCM-U11@P increased to 21.2% and 66.6%, respectively (Figure k,l). In particular, TCM-U11@P
showed the most significant cell uptake efficiency with the extension
of incubation time to 18 h (96.1%). The above flow cytometry analysis
results were completely consistent with the in vitro confocal imaging results (Figure a–f). In addition, we also verified the in vitro PDT performance of TCM-U11&Cy@P in cell experiments
(Figure S14 in the Supporting Information).
Combining all of the above in vitro experimental
results, the sequence-activated strategy with the incorporation of
U11 peptide in TCM-U11@P markedly facilitated cellular internalization
of PANC-1 cells and thereby enabled fluorescence imaging with high
fidelity.
Revealing Excellent Permeability in a Multicellular 3D Tumor
Spheroid
As mentioned above, our designed sequence-activated
nanotheranostics TCM-U11&Cy@P could synergistically enhance the
targeting ability and permeability to PANC-1 cells. With this in mind,
we chose three-dimensional (3D)-structured PANC-1 multicellular tumor
spheroids (MCTSs, size: ca. 1 mm) to simulate a PDAC tumor.[78,79] Then, we further evaluated the improved tumor targeting and permeability
of TCM-U11&Cy@P in MCTSs. By scanning along the z-axis with dual-channel emission at 650 and 830 nm, we recorded fluorescence
images in each 9 μm layer of PANC-1 MCTSs treated with TCM-DN
and TCM-U11&Cy@P. As shown in Figure a,b, TCM-DN showed a very weak fluorescence
signal. In contrast, TCM-U11&Cy@P expressed a visibly brighter
and uniformly distributed fluorescence signal in MCTSs, implying much
better targeting delivery and efficient penetration. Also, these results
further quantitatively confirmed the much better permeability of TCM-U11&Cy@P
as compared to TCM-DN (Figure S15 in the
Supporting Information). Then, we reconstructed 3D spheroid images
through the fluorescence signal of the focal planes. As observed in Figure c and Video S1, significant dual-channel fluorescent
signals were expressed in the reconstructed 360° rotation video
of the 3D-structured spheroids at both 650 and 830 nm. In addition,
the in vivo FRET process was consistent with in vitro experimental results (Figure S16 in the Supporting Information). It is believed that the
two channels (830 and 650 nm) are complementary to the imaging output in vivo and in vitro, greatly improving
particular advantages in the bioimaging applications (Figure S17 in the Supporting Information). Clearly,
these results highlighted the excellent PDAC tumor targeting and permeability
of our sequence-activated nanotheranostic TCM-U11&Cy@P.
Figure 5
Revealing the
permeability: dual-channel in vitro imaging of PANC-1
multicellular tumor spheroids. (a, b) Three-dimensional
tumor spheroid images obtained along the z-axis direction
at different depths of PANC-1 MCTSs. Scale bar = 200 μm. Note:
green signal, λex = 730 nm, λem =
830 nm; red signal, λex = 510 nm, λem = 650 nm. (c) Three-dimensional reconstruction of confocal microscopy
images of PANC-1 MCTSs. Scale bar = 200 μm.
Revealing the
permeability: dual-channel in vitro imaging of PANC-1
multicellular tumor spheroids. (a, b) Three-dimensional
tumor spheroid images obtained along the z-axis direction
at different depths of PANC-1 MCTSs. Scale bar = 200 μm. Note:
green signal, λex = 730 nm, λem =
830 nm; red signal, λex = 510 nm, λem = 650 nm. (c) Three-dimensional reconstruction of confocal microscopy
images of PANC-1 MCTSs. Scale bar = 200 μm.
Intraoperatively Mapping Human Clinical Specimens with High
Resolution
Learning from all of the in vitro and in vivo results, TCM-U11&Cy@P showed excellent
tumor permeability via programmable passive targeting, pH-induced
active targeting, and U11 peptide-mediated active targeting. All of
these results inspired us to further utilize TCM-U11&Cy@P for
mapping human clinical specimens. Therefore, we intraoperatively collected
human clinical tissue specimens containing PDAC tissues from patients
(pathologically confirmed as PDAC). Patients’ pathological
Nos. 21579 and 10583 are paraffin sections, and Nos. 00857 and 00841
are frozen sections. These sections were incubated with TCM-U11&Cy@P
(16 μM), and then, NIR fluorescence imaging was performed. With
the help of high-resolution fluorescence images, the normal tissue
and tumor tissue could be rapidly distinguished. In normal tissue,
pancreatic lobules with densely arranged normal pancreatic cells were
clearly observed (Figure a). In contrast, tumor tissue showed malignant histological
features including pancreatic cancer embolus and irregular ductlike
and tubular structures with glandularly arranged cancer cells. Learning
from the fluorescence imaging, the tumor tissue showed significant
histological and cell morphological abnormalities compared to the
normal tissue (Figure c). Synchronously, the H&E staining, a standard histopathological
examination, was further conducted. All of the results strongly verified
the pathological characteristics in NIR fluorescence imaging (Figure b,d). Compared to
commercial dye (ICG), TCM-U11&Cy@P exhibited a much higher resolution
and significant signal-to-noise (S/N) ratio, further verifying that
TCM-U11&Cy@P could map and amplify high-fidelity information in
human pancreatic slices (Figure S18 in
the Supporting Information). This high-precision and high-fidelity
imaging of TCM-U11&Cy@P provided a simple, sensitive, and rapid
way to observe the structural differences between the normal tissue
and pancreatic cancer tissue.
Figure 6
High-resolution three-dimensional fluorescence
imaging of human
pancreatic sections. We intraoperatively collect clinical tissue specimens
containing PDAC tissues from patients (pathologically confirmed as
PDAC). Fluorescence imaging (λex = 510 nm, λem = 650 nm) and H&E staining of paraffin sections (a–d)
and frozen sections (g–j) with TCM-U11&Cy@P (16 μM).
Green arrows indicate a normal pancreatic lobule (with densely arranged
pancreatic cells). Yellow arrows indicate malignant elements (irregular
ductlike and tubular structures). The blue arrow indicates a pancreatic
cancer embolus. PDAC tissue images indicate neoplastic glandular ducts
with glandularly arranged cancer cells, showing significant abnormalities
in tissue structure and cell morphology. Scale bar = 50 μm.
Three-dimensional reconstruction of confocal microscopy images of
paraffin sections (e, f) and frozen sections (k, l) along the z-axis direction at the depth of 48 μm. Scale bar
= 50 μm. Note: Patient’s pathological Nos. 21579 and
10583 for panels a–d, Nos. 00857 and 00841 for panels g–j.
High-resolution three-dimensional fluorescence
imaging of human
pancreatic sections. We intraoperatively collect clinical tissue specimens
containing PDAC tissues from patients (pathologically confirmed as
PDAC). Fluorescence imaging (λex = 510 nm, λem = 650 nm) and H&E staining of paraffin sections (a–d)
and frozen sections (g–j) with TCM-U11&Cy@P (16 μM).
Green arrows indicate a normal pancreatic lobule (with densely arranged
pancreatic cells). Yellow arrows indicate malignant elements (irregular
ductlike and tubular structures). The blue arrow indicates a pancreatic
cancer embolus. PDAC tissue images indicate neoplastic glandular ducts
with glandularly arranged cancer cells, showing significant abnormalities
in tissue structure and cell morphology. Scale bar = 50 μm.
Three-dimensional reconstruction of confocal microscopy images of
paraffin sections (e, f) and frozen sections (k, l) along the z-axis direction at the depth of 48 μm. Scale bar
= 50 μm. Note: Patient’s pathological Nos. 21579 and
10583 for panels a–d, Nos. 00857 and 00841 for panels g–j.This high-fidelity imaging also made it an ideal
contrast agent
for three-dimensional (3D) fluorescence imaging. After incubation
with TCM-U11&Cy@P, high-resolution 3D fluorescence images were
obtained with a Leica TCS SP8 instrument. As shown in Figure e,f, and Video S2, TCM-U11&Cy@P exhibited strong NIR fluorescence
signals in the clinical tissue specimens, thus achieving high-fidelity
mapping from different perspectives. Importantly, this 3D fluorescence
imaging could also provide more details of longitudinal information.
In order to further verify the imaging effect and clinical application
value, we also conducted the above imaging experiments on frozen sections.
As expected, similar imaging results were also observed with frozen
sections (Figure g–l
and Video S3). All of these results demonstrated
that TCM-U11&Cy@P made a breakthrough for rapidly distinguishing
human normal tissue and pancreatic cancer tissue via high-fidelity
fluorescence imaging.
Conclusions
In summary, we focused
on engineering a programmable targeting
strategy of fluorescent nanotheranostics for real-time tracking the
delivery across PDAC-specific physical barriers and efficient uptake
of deep tumor cells. For the first time, we developed sequence-activated
fluorescent nanotheranostic TCM-U1&Cy@P for human pancreatic cancer
with an enhanced multitargeting capability: (i) programmable passive
targeting, (ii) tumor pH-induced active targeting, and (iii) U11 peptide-mediated
active targeting. Ultimately, the released TCM-U11 particles overcome
the limitation of dense stroma, allowing for the direct interaction
with PDAC cells in the deep tissue for activatable PDT to ablate tumors.
The multicellular tumor spheroids and in vivo assessments
clearly demonstrated that TCM-U11&Cy@P was equipped with potent
PDAC-tumor targeting, deep delivery, and phototoxicity. Impressively,
FRET-based dual-channel activatable fluorescence was employed for
monitoring the programmable targeting process. Most importantly, accompanied
by bright NIR emission from the released AIE nanoaggregates inside
tumor cells, TCM-U11&Cy@P successfully mapped human clinical specimens
with high resolution. The programmable tumor targeting ability of
TCM-U11&Cy@P made the breakthrough of tracking across PDAC-specific
physical barriers in real time and thereby displayed enhanced tumor
permeability. Our study presents a new visualization strategy for
the in vivo application of intelligent nanotheranostics,
paving a new pathway for pancreatic carcinoma.
Authors: M A Tempero; J Berlin; M Ducreux; D Haller; P Harper; D Khayat; H-J Schmoll; A Sobrero; E Van Cutsem Journal: Ann Oncol Date: 2011-01-03 Impact factor: 32.976
Authors: Amit Sharma; Min-Goo Lee; Miae Won; Seyoung Koo; Jonathan F Arambula; Jonathan L Sessler; Sung-Gil Chi; Jong Seung Kim Journal: J Am Chem Soc Date: 2019-09-24 Impact factor: 15.419
Authors: H Cabral; Y Matsumoto; K Mizuno; Q Chen; M Murakami; M Kimura; Y Terada; M R Kano; K Miyazono; M Uesaka; N Nishiyama; K Kataoka Journal: Nat Nanotechnol Date: 2011-10-23 Impact factor: 40.523
Authors: Weina Gao; Nikki K Lytle; Yu Shi; Peiwu Huang; Xiao Yuan; Amanda M Dann; Maya Ridinger-Saison; Kathleen E DelGiorno; Corina E Antal; Gaoyang Liang; Annette R Atkins; Galina Erikson; Huaiyu Sun; Jill Meisenhelder; Elena Terenziani; Gyunghwi Woo; Linjing Fang; Thom P Santisakultarm; Uri Manor; Ruilian Xu; Carlos R Becerra; Erkut Borazanci; Daniel D Von Hoff; Paul M Grandgenett; Michael A Hollingsworth; Mathias Leblanc; Sarah E Umetsu; Eric A Collisson; Miriam Scadeng; Andrew M Lowy; Timothy R Donahue; Tannishtha Reya; Michael Downes; Ronald M Evans; Geoffrey M Wahl; Tony Pawson; Ruijun Tian; Tony Hunter Journal: Nature Date: 2019-04-17 Impact factor: 49.962