Open Access Article
Zihnil Adha Islamy Mazrad‡
a,
Eun Bi Kang‡b,
Nuraenia,
Gibaek Leeb,
Insik In
*ac and
Sung Young Park
*ab
aDepartment of IT Convergence, Korea National University of Transportation, Chungju 380-702, Republic of Korea. E-mail: parkchem@ut.ac.kr
bDepartment of Chemical and Biological Engineering, Korea National University of Transportation, Chungju 380-702, Republic of Korea
cDepartment of Polymer Science and Engineering, Korea National University of Transportation, Chungju 380-702, Republic of Korea
First published on 10th February 2017
Here, we report novel thermo-responsive fluorescent nanoparticles of carbonized poly(N-isopropylacrylamide) (PNIPAAm) through two pathways, partial carbonized PNIPAAm (F-PNIPAAm) and full carbonized PNIPAAm (FNP) acid treatment. The carbonized PNIPAAm generated different properties depending on acid treatment time to control the lower critical solution temperature (LCST) behaviors as a biosensor based on a fluorescence on–off system. Furthermore, the FNP–PNIPAAm also showed reversible capability based on fluorescence intensity, with a high fluorescence signal observed at room temperature (25 °C) but quenching at physiological temperature (37 °C). H-NMR, FT-IR, X-ray dispersion (XRD), and X-ray photoelectron spectroscopy (XPS) confirmed the associated chemical moieties of FNP–PNIPAAm and FNP. After confirming the cytotoxicity of the prepared material, we carried out in vitro bio-imaging studies using MDAMB, A-549, and MDCK cells by confocal laser-scanning microscopy. Therefore, we successfully established a convenient, rapid, and ecofriendly synthetic approach to the synthesis of FNPs based on PNIPAAm. These FNPs exhibited tunable luminescence properties, high aqueous stability, and low cytotoxicity, suggesting potential applications in bio-labeling, bio-imaging, and optoelectronics.
Recently, fluorescent agent-based thermo-responsive materials resulted big attention in wide range of areas because of their potential applications. These studies have demonstrated sensitive and reversible thermo-stimulus for fluorescence-color/on–off switching characteristics, and the fluorescence parameters (intensity, wavelength, and lifetime) showed high sensitivity and linearity depending on the temperature. This approach have been found within biomedical uses, including the release of drugs at body temperature as a common method in thermo-responsive studies, and their use in biomedical applications will have a definite impact in the medical field.20 Poly(N-isopropylacrylamide) (PNIPAAm) is a well-known temperature-sensitive linear polymer that exhibits a lower critical solution temperature (LCST) of approximately 32 °C in aqueous solution, becoming less soluble and coagulating at temperatures higher than 32 °C to form a hydrophobic material.21 Considering all of these advantages, PNIPAAm play an important role in biomedical applications such as in drug delivery systems, controlled release of drugs, and tissue engineering.22–24 Moreover, the PNIPAAm chain consists of abundant amounts of carbon, nitrogen, and oxygen, leading to possess fluorescent properties through the acid treatment owing to simultaneous partial carbonization and thereby affecting LCST behaviors in the context of increased temperatures.
Inspired from thermo-sensitive PNIPAAm and the electronic response of carbonized material, we aimed to create new desirable agents possessing the capacity for application as a fluorescence on–off biosensor and bioimaging agent.14 Generally, PNIPAAm does not show photoluminescence behavior during excitation; however, after acid treatment, carbonized PNIPAAm exhibits bright blue fluorescence due to surface functionalization by carboxylic acid or amine groups in the NIPAAm chain. PNIPAAm has been extensively studied as a thermoresponsive polymer that acts as a reversible switch between hydrophilic and hydrophobic states in response to temperature change. This polymer exhibits an LCST that undergoes a phase transition at 32 °C in aqueous solution.22–25 Moreover, PNIPAAm transforms from the water-swollen state to the globular state when heated to above its LCST in aqueous solution.
In this work, we prepared two materials by controlling the carbonization times of PNIPAAm to obtain thermo sensitive fluorescent nanoparticles. We then attempted to establish a simple, low-cost strategy for the synthesis of temperature-sensitive FNPs prepared using PNIPAAm as a precursor material with a defined dehydrating system to control the time of the reaction. Carbonization was carried out for 1 min or 1 h using two different acid treatments, confirming that the treatment will help to maintain LCST behaviors of PNIPAAm. These carbonized nanoparticles produced a bright blue fluorescence with good solubility in water, could be effectively served in bio-labeling, bio-imaging, and optoelectronics.
600) was prepared as previously described.21
O stretching vibration peaks at 3225 and 1700 cm−1, respectively, suggestive of the appearance of amine and carboxyl linkages of FNP–PNIPAAm.27,28 In X-ray diffraction (XRD) patterns as shown in Fig. 1c, unmodified PNIPAAm shows a primary crystalline peak centered at around 2θ = 20°, including an amorphous peak at 2θ = 12°. After hydrothermal treatment, the intensity of the amorphous peak was increased by reducing the crystalline peak, indicating that the PNIPAAm was partially oxidized into FNP–PNIPAAm, while the FNP amorphous peak was observed at around 2θ = 20–40°, confirming the complete carbonization after prolonged acid treatment.29 Fig. S1† show Raman studies of PNIPAAm partial and complete acid treatment, indicating the presence of peak at area 1370 nm as D band and 1540 nm as G band. G/D bands imply sp3 and sp2 carbon contents, which is used to correlate different ratios of the sp2/sp3 to understand the existence of defects in the carbonized material.29 Regarding the G/D band peaks, we conclude full carbonization of PNIPAAm gives rise content of sp2, implying more defect compared with partially carbonized PNIPAAm.
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| Fig. 1 1H-NMR (a) and FTIR (b) spectra of PNIPAAm, FNP–PNIPAAm, and FNP (c) the X-ray diffraction (XRD) patterns in the range of 1 to 80° for PNIPAAm, FNP–PNIPAAm, and FNP. | ||
To evaluate the thermo-responsive nature of FNP–PNIPAAm and FNP, we observed their absorption properties using UV-Vis spectroscopy at three temperatures (25, 30 and 37 °C). The UV-Vis spectra exhibited an absorbance peak at 300 nm (Fig. 2a and b), which referred to as the π–π* transition of the carbon bond derived from the PNIPAAm polymer chain.30 Fig. 2a shows the absorption curve of FNP–PNIPAAm increased with enhancement temperature because of the reducing transmittance of sample, implication soluble-to-insoluble phase transition in an aqueous medium at around 37 °C, which was not observed of the FNP. To compare the LCST behaviors (Fig. 2c) of our samples, we observed FNP–PNIPAAm and FNP behavior at 20 to 60 °C. The FNP–PNIPAAm produced the same LCST behavior about 30 °C as PNIPAAm, whereas fully carbonized FNP did not show the same behaviors owing to disappearance of the natural structure of the NIPAAm unit. These data clearly confirmed that after acid treatment of FNP–PNIPAAm for 1 min, some partial carbonized PNIPAAm was present, which helped to maintain the LCST behaviors for further applications.
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| Fig. 2 UV-Vis spectra of FNP–PNIPAAm (a) and FNP (b) at different temperatures. (c) LCST behaviors of PNIPAAm, FNP–PNIPAAm, and FNP at 20–60 °C. | ||
Carbonized materials usually contain a mixture of sp2 type π bonding and the light emission from such carbon system are a consequence of the geminate recombination of localized electron–hole (e–h) pairs in sp2 clusters, which essentially behave as luminescence centers or chromophores. Although the emission energy bandgap depends on the size, shape, and fraction of the sp2 domains, tunable light emission can be achieved by controlling the nature of carbonization.31 These carbonized PNIPAAm molecules showed fluorescence behaviors due to a quantum effect including different emissive traps on the surface of FNP.32 To confirm the photoluminescence (PL) properties of FNP–PNIPAAm, we first performed experiments under a UV lamp at 365 nm, observing blue fluorescence emission. By evaluating the PL spectra of FNP–PNIPAAm, we found that the highest emission intensity was centered at 385 nm when the excitation energy was 340 nm (Fig. 3). Furthermore, as shown in Fig. 3a, we analyzed the effects of room temperature and physiological temperature for FNP–PNIPAAm; higher fluorescence emission was observed at room temperature, and there was no detectable fluorescence found at physiological temperature. The quenching mechanism of the FNP–PNIPAAm, which was not observed for FNP (Fig. 3b), could be attributed to the formation of micelle nanoparticles via hydrophilic and hydrophobic interactions maintained by partial carbonizing of PNIPAAm at high temperature; however, at room temperature, no fluorescence off signal occurred, which could be attributed to the hydrophilic nature of the NIPAAm unit.33 In addition, we have investigated the study to obtain the carbonized PNIPAAm dependent on different acid treatment time (10–50 min). Fig S2a† shows slightly increase dependent on increasing reaction time. Otherwise after increase the temperature (37 °C), a quenching was not seen at 50 min treatment due to the losing of NIPAAm structure effect by fully carbonized treatment (Fig. S2b†). Furthermore, Fig. S3† represent the fluorescent behavior of the partial carbonized PNIPAAm observed at 10–50 °C to understand the effect of temperature range. The sharp quenching effect has start at 40 °C whereas at 10–30 °C there is no clearly fluorescence changes were observed, it means the effect to fluorescence related to LCST value of PNIPAAm. This mechanism provides a responsiveness that may be useful for temperature-triggered detection of tumor cells. The reversible temperature-triggered behavior shown in Fig. 3c was confirmed through three cycles of reversible fluorescence quenching achieved by adjusting the temperature from 25 to 37 °C. The fluorescence remained stable as the temperature changed through several cycles, indicating the thermostability of FNP–PNIPAAm.
The DLS data also showed that the diameter increased as the temperature increased because of coagulation, confirming the existence of PNIPAAm properties after acid treatment in FNP–PNIPAAm (Fig. 4a and b). In contrast, fully carbonized FNP showed almost the same particle sizes as the temperature increased, implying loss of the thermosensitivity of PNIPAAm. TEM images of FNP–PNIPAAm (Fig. 4c) showed cylinder-shaped particles with small defects and a comparatively narrow size distribution (150–200 nm) because the short carbonizing time preserved the PNIPAAm shape after acid treatment (Fig. S4†). In contrast, FNP (Fig. 4d) were dot shaped after full acid treatment, with the lattice separations of those carbonized materials (∼0.285–0.33 nm), confirming the presence of graphene carbon structures indicative of internalized carbon particles.34
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| Fig. 4 Dynamic light spectroscopy (DLS) of FNP–PNIPAAm (a) and FNP (b) at different temperatures. TEM images of (c) FNP–PNIPAAm and (d) FNP. | ||
The survey scans of XPS results were also consistent with the FT-IR analysis. Based on the XPS analysis (Fig. 5a), the as-prepared acid-treated PNIPAAm and FNP contained a high percentage of oxygen atoms compared with PNIPAAm because of the functionalization of carboxylic or amine groups in the FNP–PNIPAAm chain. Next, the C1s core level spectrum of FNP–PNIPAAm and FNP showed a considerable degree of oxidation with four components corresponding to carbon atoms with different functional groups, i.e., oxygenated C (C
O) at 287.5–292 eV, C–C bonds (284.5 eV), C
C bonds (284 eV), and C–N bonds (285.4 eV), and a prominent π–π* transition peak appeared at 292 eV, showing the presence of some carboxylic and hydroxyl groups on the carbonized FNP.14 Fig. 5b shows the elemental composition of PNIPAAM, FNP–PNIPAAm, and FNP in C1s analysis; the results showed increased percentages of sp2-type carbons in FNP.
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| Fig. 5 (a) Survey scan of PNIPAAm, FNP–PNIPAAm, and FNP, deconvoluted C1s peak of PNIPAAM, FNP–PNIPAAm and FNP. (b) XPS-based elemental carbon (C1s) analysis of PNIPAAm, FNP–PNIPAAm, and FNP. | ||
To visualize the fluorescence state in cell, we used confocal images of FNP–PNIPAAm and FNP monitored with a CLSM (Fig. 6a), which can be used for cellular imaging and diagnosis. For fluorescence microscopic images, the corresponding cells were loaded with both bioimaging agents, showing emission of blue and green fluorescence after 4 h of incubation after excitation with their corresponding excitation wavelength. Notably, the nanoparticles were accumulated within the cell cytoplasm randomly owing to nonspecific delivery of FNPs. The results from confocal images support the use of these agents as strong candidates for cellular imaging and diagnosis. To evaluate the cytotoxic behavior of FNP–PNIPAAm, we examined the in vitro cytotoxicity in three cell types, including MDAMB, A549, and MDCK cells. Our findings confirmed that this material was not toxic, with ∼100% cell viability observed after treatment with FNP–PNIPAAm at different concentrations. Similar results were observed for FNP. Thus, these materials may be applied as nontoxic material for biological purposes (Fig. 6b and S5†).35
This work can control the fluorescent behavior through carbonization time and obtain the reversible behavior by temperature change based on PNIPAAm and thermoresponsive polymer. Some studies reported that unique fluorescent properties can be from graphene carbon nanodots treated by ultra-sonication, which generate visible emission with near-infrared (NIR) excitation.36 But this FNPs based carbonized PNIPAAm showed intrinsic emission which can quench based LCST behavior dependent on carbonization time, resulting reversible fluorescent on/off system based temperature change.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra25104h |
| ‡ These authors equally contributed to this work. |
| This journal is © The Royal Society of Chemistry 2017 |