Xuejing Wang‡
,
Yinyan Yuan‡,
YiXiao Sun,
Xue Liu,
Mingze Ma,
Renyin Zhang and
Feng Shi*
College of Life Sciences, Shihezi University, Shihezi 832003, China
First published on 26th September 2022
The development of luminescent materials greatly affects the development of fluorescence imaging technology. The preparation of carbon dots (CDs) with high photoluminescence quantum yield (PLQY) in the solid-state is challenging due to excessive resonance energy transfer (RET) and direct π–π interactions. In this study, we synthesized carbon dots that exhibit green fluorescence (GCDs) with absolute PLQYs up to 35.65% in one step by a microwave-assisted method. In the solid-state, the absolute PLQY reached 19.25%. Then, the GCDs were mixed with soluble starch in appropriate proportions, which improved the adsorption and dispersion of the GCDs and greatly reduced the cost of the fingerprint powder, and increased the absolute PLQY of the fingerprint powder to 41.75%. Finally, we prepared GCDs for preliminary fabrication of luminescent films, and the GCD-starch powder was successfully applied to high-quality latent fingerprint (LFP) imaging. The related properties of GCDs and the LFP detection performance of fingerprint detection powders prepared by GCDs were studied in detail. The results showed that the LFP system developed with GCDs-starch powder visualized LFPs with high definition and contrast under different conditions, and GCDs had potential for application in light-emitting devices. This study developed a new type of solid-state luminescent CDs and demonstrated that these GCDs have great application potential for LFP detection. This study may also provide inspiration for other applications based on efficient solid-state fluorescence.
Detection of latent fingerprints using fluorescent dyes is a commonly used method. Fluorescent dyes or photoluminescence nanomaterials are sprayed on the fingerprints, and LFP imaging is performed with the contrast from fluorescent signal intensity under excitation light.9 For example, upconversion nanoparticles,10 quantum dots,11 and organic dyes12 have been used for LFP imaging. Although LFP imaging can be realized by using fluorescence, there are many fluorescent materials, such as semiconductor quantum dots and heavy metal dyes, which cause great harm to the environment or exhibit fluorescence quenching due to aggregation in the solid-state.13 This greatly limits their application in LFP imaging recognition. Therefore, it is necessary to prepare a fluorescent material with good environmental compatibility and bright fluorescence in solid-state for LFP imaging.
Recently, carbon dots (CDs) have attracted attention in many fields due to their excellent properties, such as easy preparation, high photostability, strong photoluminescence, good biocompatibility, environmental friendliness, and low preparation cost, which also have applications in LFP imaging.14,15 For example, Chen et al. synthesized red fluorescent carbon dots by a hydrothermal method and dissolved them in dilute hydrochloric acid. Spraying this solution results in a distinct red fluorescent LFP image.16 Compared with traditional organic dyes and semiconductor quantum dots, CDs have been more widely used in optical sensing, drug delivery, bioimaging and other fields due to their metal-free nature, low toxicity and good biocompatibility.17–19 However, most CDs exhibit fluorescence in solution but may exhibit aggregation-induced fluorescence quenching due to resonance energy transfer or direct π–π interactions; this limits the application of CDs in some solid-state imaging fields, such as latent fingerprint imaging detection and manufacture of optical devices.20 For LFP imaging, it is important to provide clear fingerprint images.9 While ensuring proper adsorption between fingerprinting powders and LFPs, it is important to realize proper dispersion of the powder particles and overcome aggregation-caused quenching (ACQ) to provide high fluorescence quantum yields (QYs) and clear LFP images.
In this study, we used a simple one-step microwave-assisted method to synthesize GCDs exhibiting absolute QYs up to 35.65%. In the solid-state, the absolute QY reached 19.25%, and the absolute QY of the fingerprinting powder was as high as 41.75%. These QYs are higher than those of some organic fluorescent dyes and rare-earth metal quantum dots and much higher than those of many solid-state luminescent CDs previously reported. Moreover, fabrication of the luminescent films further proves the great potential of these CDs in various applications involving solid-state luminescence and strong fluorescence.
Fig. 2 (a) TEM image; ((a), inset) HRTEM image; (b) GCD particle size distribution; ((b), inset) GCDs under sunlight and ultraviolet light. |
To clarify the structure and properties, various techniques were used to characterize and analyse the prepared GCDs and GCD-starch powders. The morphology of the GCDs was observed by transmission electron microscopy (TEM) and high-resolution transmission electron microscopy (HRTEM) (Fig. 2a). The TEM image showed that the GCD particles were quasi-spherical. The TEM images were imported into Nano Measurer 1.2, and the sizes of 300 GCD particles were measured. Based on this, the particle size distribution of the GCDs was determined (Fig. 2b), and the average particle size was calculated to be 1.51 ± 0.48 nm. In addition, high-resolution microscopy images (inset of Fig. 2a) showed that the GCDs exhibited lattice fringes with an interplanar spacing of approximately 0.21 nm, which corresponded to the (100) plane of graphitic carbon.22 The results from dynamic light scattering showed that the average GCD particle size was 16.37 nm; this differed considerably from the electron microscope image, which may have been due to aggregation of GCDs to form nanoclusters.23 The GCDs showed a broad and strong peak at approximately 21° (Fig. 3a), which again indicated the presence of a disordered graphitic structure and formation of carbon dots.24–27
Fig. 3 (a) XRD pattern of GCD powder; (b) UV absorption curves of starch, GCDs, and GCD-starch powder. |
To determine the optical properties of GCDs and GCD-starch powder, the UV-Vis absorption spectra of starch, GCDs, and GCD-starch powder were compared, as shown in Fig. 3b. The main absorption peak for GCDs was seen at approximately 395 nm. When the starch and GCDs were combined, the peak was blueshifted to approximately 375 nm. When nanoparticles gather in the solid state, the molecular orbitals of the GCDs overlap each other. This overlap reduces the average band gap of the GCDs and causes a redshift of the absorption spectra.28 However, when GCDs were dispersed into a 40-fold excess of starch, the distance between GCDs increased obviously, the redshift was inhibited, and the absorption curve exhibited a blueshift. The blueshift of the peak in Fig. 3b indicated a strong interaction between the GCDs and the starch.
As shown in Fig. 4a, the GCDs showed excitation-independent photoluminescence (PL) emission in ethanol solution with an emission peak at approximately 495 nm; the excitation spectrum of the GCDs was also determined (Fig. 4b), which showed that the optimal excitation wavelength of the GCDs was at approximately 395 nm. The inset of Fig. 5b showed that starch itself did not fluoresce, but GCD-starch retained the fluorescent properties of the GCDs. For example, GCD-starch powders were dispersed in ethanol, and PL spectroscopy was performed. As shown in Fig. 5a, the position of the emission peak was almost unchanged by increasing the excitation wavelength, which indicated that both GCDs and GCD-starch powders exhibited excitation-independent PL emission in solution. Fig. 5b shows the excitation spectrum of the GCD-starch powder, and the results were consistent with the previous analysis.
Fig. 4 (a) Emission spectra of GCDs at different excitation wavelengths; (b) excitation spectra of GCDs at optimal emission wavelengths. |
Generally, after CDs solution is dried into a powder, the fluorescent intensity becomes very weak due to the ACQ. A high PLQY is very important for the development of various applications for CDs. However, the PLQY of solid-state CDs is relatively low compared to liquid-state fluorescence due to the ACQ effect. When the GCD solution was dried into a powder, its fluorescence intensity decreased but remained at a high level. In contrast, the PLQY of GCDs-starch powder measured with 395 nm excitation and an integrating sphere was approximately 41.25%, which is much higher than the PLQYs of many other solid-state CDs and fingerprint detection powders (Table S1†). Generally, due to the quenching effect of aggregated fluorescence, solid-state carbon dots emit weakly or even no fluorescence, which leads to the inability of carbon dots to be directly applied to fingerprint detection. However, when a large amount of starch is combined with carbon dots (CDs), the CDs in the aggregated state are dispersed, and the distance between CDs increases, thereby overcoming the aggregation-induced fluorescence quenching. Similar methods also use silica for dispersion,29 chemical doping dilution,13 and so on.
The FTIR spectrum of the GCDs (Fig. 6) showed stretching vibrations for O–H at 3383 cm−1, C–H at 2919 cm−1, CC/CO at 1594 cm−1, N–H at 1455 cm−1, C–N at 1400 cm−1, C–S at 1472 cm−1, SO at 1475 cm−1, and C–O at 1300 cm−1.28,30–33 These peaks were also observed in the FTIR spectrum of GCDs-starch, which combined the FTIR peaks for starch, GCDs-starch powder, and GCDs and indicated that GCDs were wrapped around the starch granules (Fig. 6). Therefore, the abovementioned functional groups of GCDs provided the adsorption peaks for the GCDs and starch and fingerprint residues.
The full-range X-ray photoelectron spectra (XPS) (Fig. 7a) demonstrated peaks for C 1s (284.77 eV), N 1s (399.27 eV), O 1s (531.27 eV) and S 2p (163.13 eV) binding energies. The XPS spectrum showed that the elemental contents for C, O, N and S (inset of Fig. 7a) were 76.13%, 19.45%, 2.05% and 2.37%, respectively. In the high-resolution XPS spectrum (Fig. 7b–e), the C 1s band was deconvoluted into four peaks corresponding to the sp2- and sp3-hybridized carbons of C–C/CC (284.6 eV), C–O/C–S/C–N (285.1 eV), CO (288.5 eV), and CO/CN (288.1 eV) moieties.27,34,35 The N 1s band was deconvoluted into three peaks at 398.9, 399.5, and 400.0 eV, which represented CN, C–N–C, and N–H moieties,36 respectively, indicating that N atoms were present in the GCDs. The O 1s band contained four peaks at 530.8, 531.5, 532.6 and 535.5 eV, representing C–O, OS/CO, CO/C–O and C–OH/C–O–C.37–39 The S 2p band contained four peaks at 162.9, 163.9, 168.3 and 169.3 eV, representing C–S, S 2p1/2, SO3 and SO,30,32,40 which clearly indicated the presence of S atoms in the GCDs. These XPS results were consistent with those obtained by FTIR, and the FTIR and XPS investigations indicated that –OH and –NH2 functional groups on the surfaces of the GCDs improved their electronic properties, hydrophilicity, and stability.
Fig. 7 (a) XPS survey spectrum of GCDs; (b–e): N 1s, C 1s, O 1s, and S 2p high-resolution spectra of GCDs; “raw” indicates the data without fitting, and “fitting” indicates data after fitting. |
The abundant functional groups on the surfaces of CDs are the sources of their high fluorescence intensities, and FTIR and XPS investigations indicated the presence of –OH and –NH2 functional groups on the surfaces of GCDs. It is well known that surface defects introduced by N and S co-doping affect the graphitization degree of CDs.30,33 Experiments showed that the GCDs and GCDs-starch prepared in this study exhibited strong fluorescence, and our GCDs-starch powder formed a high contrast with the background for LFP detection.
To test whether the GCD-starch powder can be used for LFP imaging, a glass plate was first selected as a substrate for fingerprints and LFP detection. Before performing LFP imaging, we optimized the mass ratio of the carbon and nitrogen sources (Fig. 8a) and the amount of sodium hydroxide added (Fig. 8b) during preparation of the GCDs according to the fluorescence intensities of the GCDs. Finally, based on the relative PLQY of the GCD-starch powder, the quality of latent fingerprint images was optimized for the mass ratio of the GCDs and starch (Fig. S3†). The quality of latent fingerprint images was evaluated based on the feature points found in the resulting latent fingerprint images (S4 fingerprint images at various scales). It was found that the GCD-starch powder with a mass ratio of 1:40 had a higher relative quantum yield and clearly enabled observation of the characteristic points of various fingerprint images.
Fig. 8 (a) GCD emission spectra for different C/N ratios; (b) GCD emission spectra of GCDs with different amounts of NaOH added. |
As shown in Fig. 9, LFPs were successfully detected on glass (Fig. 9a). Due to the high contrast of the fluorescence signal, all of the characteristics and primary structures of the fingerprint, such as the pattern, (Fig. 9b (1)) core point, (Fig. 9b (2)) triangle point, and (Fig. 9b (3)) pattern line, and number of lines can be clearly identified. As we all know, that secondary feature points give fingerprints their uniqueness, which provides the most important identifying information for accurate fingerprint analysis.28 These feature points can be clearly observed in Fig. 10c and are marked as the (1) bifurcation point, (2) endpoint, (3) isolated point, (4) short line, (5) ring point, and (6) bifurcation point. In general, although the three-level structures of fingerprints cannot be used alone to identify a LFP, when certain defects and/or second-level signal ambiguities occur, the third-level feature points provide important reference information for fingerprint identification and matching. In the fingerprint images we obtained, seven scars with different morphologies (Fig. 9a) were found and assigned with three grades. The latent fingerprint image was compared with the fingerprint image of the fingerprint supplier (S5). It was found that the overall and local characteristics of all features in the LFP corresponded, and the similarity was high. Two fingerprints often have the same overall characteristics, but the nodes of fingerprints cannot be completely the same. The figure shows that all of the feature points were identified on the fingerprint image, which also confirmed that the powder obtained in this study can be used for LFP identification. The image of the LFP on the glass plate was not processed by expensive instruments such as a confocal fluorescence microscope; a very clear picture was obtained, and the tertiary information of the fingerprint was observable. Only about 0.25 mg GCDs are needed, a clear fingerprint can be obtained.
Fig. 9 (a) LFP on a glass plate shown with GCDs-starch (1:40); (b) LFP primary structure; (c) LFP secondary structure. |
Fig. 10 (a) LFP on a glass plate; (b) LFP on a plastic bottle cap; (c) LFP on a mobile phone screen. |
To test the performance of GCD-starch powder for LFP imaging, as shown in Fig. 10, several different substrates commonly used in daily life were used for LFP imaging, such as bottle caps and mobile phone screens. The superior performance of the GCDs-starch powder in LFP imaging was proven by observing the fingerprint clarity details. The results showed that most of the details and tertiary features of fingerprints were clearly presented by our synthesized GCD-starch powder, indicating that the GCD-starch powder prepared in this study can be applied to LFP identification.
Finally, a luminescent film synthesized from GCDs also has high fluorescence and emits bright green fluorescence under ultraviolet excitation, indicating that the GCDs involved in this experiment also have certain application prospects for manufacturing of light-emitting devices.
Compared with previous reports on LFP fluorescence detection, our current work has made progress in the following ways. First, the low-cost GCDs exhibited a maximum of 35.75% PLQY in ethanol and a 19.25% PLQY in the solid-state. After mixing with starch, the resulting solid exhibited a maximum PLQY of 41.75%. Second, the fluorescent colour of our phosphor is close to green, which can be easily distinguished from the common blue background fluorescence, so it effectively improves the signal accuracy of the dyed LFP. Third, the preparation of GCD-starch powder and LFP imaging process is simple, fast, portable, and widely compatible and are far superior to traditional procedures such as fumigation. By comparing the similarities between the LFP feature points and those of the sample control, the fingerprint was easily and clearly identified. Finally, our material shows good latent fingerprint imaging ability on other materials, such as plastic bottle caps, mobile phone screens and other objects commonly used in daily life, which confirms that our materials and methods can be applied to practical LFP detection and imaging. The luminescent film synthesized from GCDs emits bright green fluorescence upon excitation with ultraviolet light, indicating that the GCDs involved in this experiment also have certain application prospects in the fabrication of light-emitting devices.
Footnotes |
† Electronic supplementary information (ESI) available. See https://doi.org/10.1039/d2ra05397g |
‡ Equal contribution. |
This journal is © The Royal Society of Chemistry 2022 |