Open Access Article
Soumen
Ghosh
,
Aayush
Anand
and
Subrata
Chattopadhyay
*
Department of Chemistry, Indian Institute of Technology Patna, Bihta, Patna 801106, Bihar, India. E-mail: sch@iitp.ac.in
First published on 27th March 2025
Developing nonconjugated polymer dot-based sensors with high quantum yield for a targeted application is a challenging research field. Herein, we report the synthesis of a zwitterionic polymer dot (PD PAMAM 2.5, average diameter 12 nm), which contains a poly(aminoamide) core and amine and acid groups on the surface. The molecular structure and functionalities of the polymer dot were carefully established using various spectroscopic techniques, including NMR, FTIR, and XPS. The polymer dot revealed greenish blue/aqua emission (λmax = 470 nm) with a quantum yield of 28%. The mechanism for the synthesis of polymer dot with respect to its structure and fluorescence property was examined using a combination of techniques, including NMR, zeta potential and fluorescence spectrometry. The application of the fluorescent polymer dot for the selective detection of 2,4,6-trinitrophenol was studied in detail. The limit of detection was determined to be 0.77 nM, which was the best value among the current state-of-the-art. Furthermore, application of the polymer dot in real life scenarios was demonstrated using real life wastewater samples and a paper-based strip-test method.
CPDs are formed from conjugated polymer networks. Owing to the presence of traditional conjugated fluorophores, conjugated polymer dots (CPDs) have excellent fluorescent properties with high fluorescence intensities, high quantum yields, multicolor fluorescence, and a clear luminescence mechanism. However, the same structural backbone results in poor water solubility and higher toxicity for practical applications, such as chemical sensing and biological analysis. Besides, the preparation of conjugated polymer dots involves multistep synthetic routes and the use of environmentally harmful organic chemicals and solvents.14–16
Therefore, the development of nonconjugated polymer dots (NCPDs) arises as a fascinating research topic. NCPDs are composed of non-conjugated polymeric backbones, containing various sub-fluorophores, such as double-bonded heteroatoms (C
O, C
N, and C
S) and amine groups.12 In the literature, several polymeric backbones are reported to develop NCPDs, which include polyethyleneimine, polyvinyl alcohols, polylactic acid, polyacrylamides, polyacrylates, polyamides, and polyurea.13,17–21 Such polymer backbones result in better water solubility, but at the same time nonconjugated polymer dots have lesser emission intensity and quantum yield. Though their rigid aggregated structure and crosslinking could improve the quantum yield (crosslinked enhanced emission) to a certain extent, the quantum yield of most of the reported nonconjugated polymer dots remains less than 15–20%.22–24 Therefore, it is indispensable to further explore the development of NCPDs from other non-conventional fluorescent polymer backbones and improve their luminescent properties and quantum yield for specific applications.
Herein, we report the design and synthesis of a poly(aminoamide)-based zwitterionic polymer dot. Poly(aminoamide)s are an important class of nonconventional fluorescent polymers, which exhibit fluorescent emission mainly due to n–π* transition and the formation of localized clusters via the interactions of alternating amines and amides within the network.25,26 In the past, fluorescent properties of such poly(aminoamide)s are well explored in the literature,27–32 but they are never reported in the context of nanodot synthesis. In recent years, our works have described the synthesis of different temperature and pH responsive biocompatible poly(aminoamide) based microgels for different sensing applications, which include different ions and ratiometric determination of temperature and pH.26,33,34 However, for the detection of external analytes, the limit of detection remains on the slightly higher side, which restricts their further developments. This is mainly ascribed to the low quantum yield of the poly(aminoamide) polymers and microgels (<5%). Therefore, we hypothesize that development of more structurally rigid polymer dots is probably the solution to enhance the emission intensity and quantum yield, and the presence of zwitterionic surface functionalities is definitely the key for their application in the sensing of nitro explosives.
In modern industry, nitro explosives are frequently employed in the domains of dyestuffs, insecticides, and pharmaceutical intermediates. Nitro explosives (significant raw ingredients in explosives) have also been linked to the rise in terrorist attacks that have put public safety, human health, and homeland security at risk.35,36 Therefore, trace detection of nitro explosives (especially 2,4,6-trinitrophenol) remains a very important research topic. Currently developed approaches for determining nitro explosives include proton transfer-assisted soft chemical ionization mass spectrometry and immunosensing based on surface plasmon resonance.37,38 One could argue that the practical applicability of the current approaches is limited as the approaches are costly, and require time-consuming steps that could be problematic to apply in the field.39 Thus, researchers have been quite focused on developing portable, reliable, and affordable technologies for nitro explosive detection. In recent years several fluorophores are reported to detect 2,4,6-trinitrophenol, which include graphitic nanomaterials, metal nanoparticles, MOFs, polymers, carbon dots, quantum dots, etc.40–45 However the limit of detection with polymer based sensors remains higher and very few of them are ever explored in real life test samples. Besides, polymer dots are rarely explored to detect nitro explosives. Only Liu et al. reported the use of a polyethyleneimine-based polymer dot to detect picric acid; however, the limit of detection was much higher, reported to be 0.5 μM.46 Therefore application of suitable designed polymer dots to detect such nitro explosives is indispensable.
To further confirm the functional groups and structure of PD PAMAM 2.5, detailed XPS analysis was conducted. Examining the XPS scanning spectra as a whole (Fig. 1C) reveals distinctive peaks of C 1s, N 1s, and O 1s at 285, 399, and 531 eV, respectively.48 Carbon, nitrogen, and oxygen were detected by full scan XPS analysis. Further analysis of the C 1s band at 285 eV clearly revealed different characteristic peaks, two peaks representing the C–C and C–N groups observed at 283.84 eV and 285.4 eV, respectively (Fig. 1D).49 The peak at 286.6 eV supports the formation of carboxylate ions (–COO−) on the surface of the polymer dot.50 The O
C–N (399.7 eV) peak was detected in the high-resolution N 1s spectra and the presence of surface amine is confirmed as the N–H peak can be detected in the high-resolution N 1s spectra at 398.26 eV (Fig. 1E).51 Similar deconvolution of the O 1s signal results in two peaks at 530.2 eV and 531.83 eV (Fig. 1F), which showed the existence of C
O and C–OH, respectively.50,51 All these combined spectroscopic analyses confirm the poly(aminoamide) core and presence of both carboxylate and amine on the surface of the polymer dot (PD PAMAM 2.5). Additionally, the presence of surface amine groups is confirmed by the ninhydrin test (Fig. S1†). Further, a broad peak is noted in the powder X-ray diffraction (PXRD) spectra, which is centered at around 2θ = 22° (Fig. S2†). This peak reveals the amorphous structure with highly disordered carbon and polymer chains. No graphitic peak is present at around 2θ = 26°, which suggests that the NCPDs were composed of a non-graphitized architecture.50 Additionally, the TGA thermogram (Fig. S3†) of the polymer dot reveals that the polymer dot is thermally stable at least until 200 °C, which is atypical of the thermal stability of poly(aminoamide) backbones.52–57
Further, the reaction is monitored at different time intervals by 1H and 13C NMR and zeta potential analysis to establish the mechanistic steps in the synthesis of zwitterionic polymer dot. 1H NMR analysis after 30 minutes of reaction under ambient conditions (step 1 in Scheme 1) reveals small oligomeric structures, representing 50% conversion of the acrylamide groups (via the integration ratio of three different peaks, Ib+c+d
:
Ia
:
If+g+h, Fig. S4A†), which is expected to form a tentative tetrameric form as represented by structure A in Scheme 1. Further structures formed during the hydrothermal treatment (step 2 in Scheme 1) were also analyzed by 1H and 13C NMR spectra at different time intervals to support the reaction mechanism and understand the formation of different functional groups (Fig. S4†). After 30 minutes of the hydrothermal reaction, 1H NMR reveals the formation of a polymeric core with surface acrylamide groups (structure B in Scheme 1). After 2 hours of the reaction, 1H NMR indicates the complete disappearance of surface acryl peaks, while the core remains unchanged. This indicates the hydrolysis reaction during the process. To evidence that further, the respective 13C NMR spectra are analyzed at different time intervals (Fig. S4B†). Two carbonyl carbon peaks after 2 hours of hydrothermal treatment clearly signify significant generation of acid groups on the surface (besides the existing amide groups), revealing zwitterionic surface formation (structure C in Scheme 1). Additionally, zeta potential was measured to confirm the similar appearance of negatively charged carboxylate groups on the surface. After 30 minutes and 1 hour of hydrothermal treatment, the zeta potential of the polymer dot was measured to be 17–18 mV (indicating the presence of positively charged amine groups predominantly) (Fig. S5 and Table S1†), while the zeta potential sharply drops to lower than 5 mV after 2 hours of hydrothermal reactions – supporting again the generation of significant negatively charged carboxylate groups, in addition to the existing amine groups on the surface, which consecutively supports the reaction mechanism, as described in Scheme 1.
The size and shape of the polymer dot was characterized using DLS, TEM and AFM. The DLS CONTIN plot indicates that the average diameter of the polymer dot was ∼12 nm (Fig. 2A). The TEM micrograph revealed an average size of the polymer dot as 8–10 nm (Fig. 2B). Additionally, atomic force microscopy (AFM) micrographs also supported the same (Fig. 2C). However, the size of the polymer dot as revealed in the AFM micrograph was ∼20 nm. The slightly higher size in the AFM micrograph is due to the softer nature of the polymer dot, which flattened when coated on a silicon surface, which is also supported via height profile analysis and a 3D image (Fig. 2D and Fig. S6†).
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| Fig. 2 (A) Hydrodynamic diameter of PD PAMAM 2.5, (B) TEM micrograph of PD PAMAM 2.5, (C) AFM micrograph of PD PAMAM 2.5, and (D) 3D AFM image of PD PAMAM 2.5. | ||
In general, poly(amino-amide) based hyperbranched polymers exhibit blue fluorescence at ∼410–450 nm.26,58 However, the emission spectra of the current polymer dot exhibit a λmax = 470 nm (greenish blue/aqua), revealing a clear red shift. This was studied further by measuring the emission spectra of the polymer dots formed at different time intervals of the hydrothermal process. The overall details are presented in Fig. 3B and Fig. S7.† The emission spectra of polymer dots formed after 0.5 and 1 hour of hydrothermal treatment (containing acrylamide functional moieties on the surface, Scheme 1) present a λmax = 410–420 nm, characteristic of poly(aminoamide) networks. However, after 2 and 2.5 hours of hydrothermal treatment (containing acid and amide groups on the surface, Scheme 1) the emission spectra of the polymer dot present a λmax = 470 nm, revealing a clear red shift. The CIE 1931 chromaticity diagram exhibits a clear colour change from blue to greenish blue/aqua with the changing co-ordinates from (0.15, 0.09) to (0.16, 0.24) (Fig. 3B). Therefore, it can be noted that the red shift and greenish blue fluorescent emission of the current poly(aminoamide) structure are a result of the formation of rigid polymer dots, and presence of amine and acid surface functionalities.59 Additionally the fluorescence intensity of the PD PAMAM 2.5 is dependent on the concentration; with increasing concentration its intensity increases as shown in Fig. S8,† due to aggregation induced emission. Further excitation dependent emission of the current polymer dot is studied (Fig. S9†). When the excitation wavelength is changed from 340 nm to 430 nm, the λmax of emission spectra remains nearly unchanged, while the intensity of the fluorescent peaks decreases continuously as the excitation wavelength is increased.
To assess the quenching efficiency, the quenching coefficient (KSV) was calculated using the Stern–Volmer equation:
| I0/I = 1 + KSV[Q] | (1) |
The process of static quenching was verified using the fluorescence lifetime decay curves of PD PAMAM 2.5 in the absence and presence of PA, as presented in Fig. 5B. Based on the decay parameter, the average lifetimes of PD PAMAM 2.5 in the absence and presence of PA were calculated (Table S3†). The average fluorescence lifetime of PD PAMAM 2.5 is calculated to be 6.48 ns. Addition of PA further does not change the lifetime (calculated to be 6.44 ns when the concentration of PA is 25 μM, and 6.38 ns when the concentration of PA is even increased to 100 μM). The near constant average fluorescence lifetime of PD PAMAM 2.5 in the absence or presence of PA supports the static quenching mechanism and suggests the formation of a ground-state complex between PD PAMAM 2.5 and PA. Furthermore, the static quenching mechanism is supported by the Stern–Volmer curve, as shown in Fig. 4D, which does not follow a linear curve throughout. The Benesi–Hildebrand plot shown in Fig. 5C provides additional evidence that supports the static quenching mechanism. The correlation coefficient value is R2 = 0.997 and the association constant (Ka) is derived from the linear interaction which was observed to be 7.234 × 105 M−1 between PD PAMAM 2.5 and PA (by analyzing the UV-VIS spectroscopy of PD PAMAM 2.5 in the presence and absence of PA, Fig. S13†). The creation of a robust complex between the guest (PA) and host (PD PAMAM 2.5) molecules through H-bonding is confirmed by this value.
Further to have a direct spectroscopic evidence and clarify the ground-state complex formation between PD PAMAM 2.5 and PA, the FTIR spectra (Fig. 5D) of PD PAMAM 2.5 both in the presence and absence of PA were studied. It is noted that a new peak arises at 1365 cm−1 along with the blue shift of the COO− (asymmetric) peak, which is visible at 1553 cm−1 and shifted from 1543 cm−1 in the presence of PA, which supports the formation of a ground state complex via hydrogen bonding interaction.
Besides static quenching, other types of quenching mechanisms such as fluorescence resonance energy transfer (FRET) and inner filter effect (IFE) are also established in the literature for sensing of PA. A spectral overap between the absorption spectra of PA and excitation and emission spectra of polymer dot indicates that IFE and FRET might interfere with the static quenching process. However, it is important to note that FRET is a dynamic quenching process. Therefore, consistent fluorescence lifetime of the polymer dot in the presence and absence of PA (Fig. 5B) clearly indicated the absence of the FRET mechanism. Further to reaffirm this, spectral overlap integral values between PA (abs) and PD PAMAM 2.5 (Em) are calculated using an established process,63,64 which clearly revealed the absence of significant FRET (Fig. S14†). In addition, the spectral overlap between the absorption spectra of PA and the excitation spectra of PD PAMAM 2.5 reveals the possibility of quenching through IFE and in this regard, we calculated the percentage of quenching by IFE using the Parker equation as established in the literature.65,66 The detailed calculation is tabulated in Table S4.† The results revealed that IFE contributed less than 10% of overall quenching when the concentration of PA was less than 7 μM. Even at a much higher concentration of PA (19 μM) the contribution of IFE is only 22%, clearly confirming that static quenching is the major quenching mechanism for the sensing of PA.
000 rpm. As the PL sensor could not detect any 2,4,6-trinitrophenol (PA) in the water samples, the samples were spiked with 2,4,6-trinitrophenol (PA) at 20 μM concentration level to perform a recovery test and validate the use of the polymer dot and quantify the level of PA using a standard curve. The findings are summarized in Table 1. There was good agreement between the added amounts and found values, and the obtained recoveries varied from 90% to 96%, indicating that these samples had no significant interferences. Furthermore, the relative standard deviations (RSD) of three replication determinations for each sample were between 0 and 3%, indicating excellent reproducibility and precision. As a result, it was anticipated that the PD PAMAM 2.5-based PL sensor could be successfully used to detect 2,4,6-trinitrophenol (PA) in real life water samples.
Further, a basic test paper assay is performed to validate its future use as a cheap sensor (Fig. 6). For test paper tests, a piece of paper was immersed in a sealed glass petri dish containing 10 mg mL−1 of polymer dot solution in water for 1 hour. Following that, the paper was taken from the solution and heated in an oven at a constant temperature of 60 °C for 1 hour to dry completely, which resulted in a polymer dot coated aqua fluorescent paper strip. Four different concentration doses (varying between 5 nM and 5 μM) of 2,4,6-trinitrophenol (PA) solution, such as 0.005 μM or 5 nM, 0.05 μM or 50 nM, 0.5 μM or 500 nM and 5 μM, were dripped onto distinct zones of the PD PAMAM 2.5-treated test paper. The prepared paper strip was dried for 2 hours at 60 °C before checking it under UV light. Under 365 nm UV light irradiation, the PL intensity of the four zones varied dramatically, and the intensity decreased as the 2,4,6-trinitrophenol (PA) concentration increased as noted in Fig. 6. The aforesaid findings suggested that a paper-based PL sensor for detecting 2,4,6-trinitrophenol (PA) within a wide concentration range is possible to be successfully manufactured in future. The paper sensor can be used with fingerprint lifting or imaging techniques to detect 2,4,6-trinitrophenol (PA) in homeland security and public safety applications.
Footnote |
| † Electronic supplementary information (ESI) available: Experimental and characterization details. See DOI: https://doi.org/10.1039/d5nr00455a |
| This journal is © The Royal Society of Chemistry 2025 |