Open Access Article
Mingxiu Leia,
Yanting Xiea,
Lin Chenab,
Xinghua Liua,
Yongzhen Yang
*ab,
Jingxia Zheng*ab and
Qiang Li*c
aKey Laboratory of Interface Science and Engineering in Advanced Materials, Ministry of Education, Taiyuan University of Technology, Taiyuan 030024, China. E-mail: yyztyut@126.com; zhengjingxia@tyut.edu.cn
bShanxi-Zheda Institute of Advanced Materials and Chemical Engineering, Taiyuan 030032, China
cIntervention Department of the Second Hospital of Shanxi Medical University, Taiyuan 030001, China. E-mail: liqiang8702226@163.com
First published on 27th September 2022
In order to explore the surface state modulation mechanism of carbon dots (CDs) with high quantum yield (QY) and high product yield (PY), CDs were synthesized from different carbon sources with different contents of oxygen-containing functional groups and different silane coupling agents with nitrogen-containing functional groups. The highest QY of as-prepared CDs can reach 97.32% and the PY values of CDs are all high ranging from 46.33–58.76%. It is found that the high content of C
O and pyrrolic N on the surface of CDs can endow CDs with high QY. Moreover, the PY of CDs not only depends on whether CDs have the crosslinked structure, but also is closely and positively correlated with pyridinic N. Consequently, our findings suggest that raw materials rich in carboxyl groups and amino groups are beneficial to the synthesis of CDs with high QY, and whether CDs with crosslinked structure and high content of pyridinic N decide the high PY of CDs. This work provides a theoretical guidance for large-scale synthesis of CDs with high QY and high PY.
A host of works to improve the fluorescent QY and PY of CDs have been reported and their related mechanisms also have been investigated.1,15–18 The studies showed that the QY and PY of CDs can be modulated through controlling the surface states of CDs with different functional groups from raw materials.19 Sun et al. demonstrated that N-doping with amino compounds can greatly improve the QY of N-doped blue-emitting CDs up to 94%.16 Zhang et al. synthesized a series of blue-emitting CDs with high QYs of 99% using amino compounds containing hydroxyl groups, which can easily provide N-doping and strong electron-donating hydroxyl, suggesting that the synergy between the hydroxyl and graphitic nitrogen can give rise to a much-improved radiative transition rate and ultra-high QY.15 Wu et al. prepared blue-emitting CDs from yeast extract powder including peptides, amino acids, minerals, and B-complex vitamins with abundant oxygen-containing (O-containing) functional groups by a one-step hydrothermal method at large scale, and the PY of CDs reaches up to 65.8%.17 Zhu et al. developed a rapid and facile magnetic hyperthermal (MHT) method for preparing blue-emitting Zn-CDs with QY of 55% and PY of 69% on a large scale and speculated that the enhanced production efficiency of CDs results from the intensified energy transfer of the MHT reaction process, with respect to conventional methods.14 In our previous work,20 nitrogen and silicon co-doped blue fluorescent CDs (b-CDs) with high QY of 97.32% and high PY of 52.56% for white light-emitting diodes (LEDs) were reported. Citric acid with abundant O-containing functional groups and N-[3-(trimethoxysilyl)propyl]ethylenediamine (KH-792) as the nitrogen dopant increase the electron cloud density on the surface of b-CDs, and thus promote the high QY of b-CDs.20 KH-792 with large spatial stereoscopic structure is beneficial to the improved structural stability of b-CDs, which further ensures the b-CDs with high PY.20 This work indicated that surface state played a key role in the obtainment of high QY and PY. Despite the great developments in this area, the surface state regulation mechanism of CDs with both high QY and high PY has been rarely reported. Therefore, the surface state regulation strategy for preparing CDs with high QY and high PY is essential for their future widespread utilization. It is well known that different functional groups can form various surface states during the formation of CDs, and raw materials dominate the surface structure of CDs, thus affecting the QY and PY of CDs. Therefore, it is necessary to clarify the effects of surface states on QY and PY of CDs.
Hence, the different carbon sources and silane coupling agents, with different contents of O-containing and nitrogen-containing (N-containing) functional groups, were selected to synthesize a series of blue fluorescent CDs by a hydrothermal method. On this basis, by characterizing QY, PY, the structure, composition and optical properties of as-prepared CDs, the internal relationship between the structure of raw material and QY and PY of CDs is revealed, and the surface state modulation mechanism of CDs with high QY and high PY is proposed in an attempt to provide theoretical guidance for synthesizing CDs with high QY and high PY. It was found that the QY and PY of CDs are closely related to O- and N-containing functional groups from raw materials, such as carboxyl, hydroxyl, methoxy and amino groups. The high QY of CDs is attributed to the high content of C
O and pyrrolic N on their surfaces. The CDs with the excitation independence property and long lifetime generally have high QY. The crosslinking structure is responsible for the high PY of the CDs, and pyridinic N can enhance the PY of CDs while amino N can weaken the PY of the CDs.
Secondly, to investigate synergistic influence of O- and N-containing functional groups on CDs, the mass of carbon sources (CA) was fixed, and silane coupling agents with different O- and N-containing functional groups (including KH-540, KH-602 and KH-792) were selected to synthesize different CDs (including 540-, 602- and CA-CDs) by hydrothermal method. Synthesis of 540- and 602-CDs followed the procedure for the synthesis of CA-CDs.
| Q = Qs(As/Ax)(Gx/Gs)(nx/ns)2 | (1) |
| PY = [mCDs/(mc + ms)] × 100% | (2) |
Thus, it can be seen that the QY of CDs synthesized with different carbon sources is closely related to the content of carboxyl and hydroxyl groups, and the PY values of CDs depend on whether the reactants can undergo crosslink reaction to obtain CDs with the crosslinking structure. To further explore this mechanism, the morphology, structure and optical properties of different CDs were characterized and compared as follow.
The surface functional groups of CDs from different carbon sources were characterized by FTIR spectroscopy. The results (Fig. 1g) show that the organosilane functionalization and formation of amide groups on the six types of CDs surface can be confirmed by the typical bands at 1030 and 1124 cm−1 originating from the stretching vibration of Si–O–Si, and at 1657 cm−1 arising from the –CONH– bond, which proves that carboxyl groups and hydroxyl groups in different carbon sources have undergone dehydration, condensation and crosslinking reactions with amino groups and siloxane groups in silane coupling agents.20,29 The vibration of the C
O bond from the carboxyl group is also found on the surface of CDs at 1660 cm−1. The intensity of O–H and C
O peak (relative to that of –CONH–) of CA-CDs with the highest QY is the highest, indicating that compared to other carbon sources, CA reacting with KH-792 has the highest degree of hydrolysis and form more amide bonds. Meanwhile, it proves that the QY of CA-CDs is higher than that of a-CDs is because the water molecules in the CA intensify the hydrolysis degree of KH-792 and the degree of reaction with CA.
As shown in Table S2,† the element analysis of CDs indicates all CDs from different carbon sources contain C, H, N, O and Si elements. CA-CDs has the highest QY and the highest surface oxygen content, manifesting the high content of oxygen of carbon source may contribute to the high QY of CA-CDs.15 For the full-scan XPS spectra of CDs as shown in Fig. S2,† the strong peaks of C 1s and O 1s indicate that all CDs are mainly composed of C and O elements, while relatively weak peaks of N 1s, Si 2p and Si 2s demonstrate that KH-792 involves in the formation of CDs, which introduces new surface states such as N-containing functional groups. This is consistent with the results of FTIR and element analysis. The analysis results of XPS for CDs from different carbon sources are shown in Table S3.† The element content of XPS is the percentage of element atoms on the surface of CDs. Element analysis of CDs is the mass percentage of their overall element. The change trend of the element analysis results of XPS is consistent with that of element analysis.
To in-depth analyse the relationship between the QY of CDs from different carbon sources and their surface structures, the C 1s and O 1s spectra of CDs in Fig. 1h were recorded, and the amounts of different types of chemical bonds in CDs were carried on the quantitative analysis, as shown in Table 1. The C 1s spectrum can be divided into three peaks (C
C, C–C and C
O), and the O 1s spectrum can be deconvoluted into C
O and C–OH. The increasing percentage of C
C on the surface of MA-CDs, LA-CDs, a-CDs, TA-CDs, CA-CDs and OA-CDs is consistent with the Raman results. With the increased QY values of CDs, both the peak intensity and percentage composition of C
O on the surface of CDs have obvious increased in Fig. 1h and Table 1. Thus, it can be suggested that the content of C
O bond and the QY of CDs have an obvious and distinct relationship. Therefore, with the gradually increase of the content of C
O bond, the oxidation degree on the surface of CDs enhances gradually, their surface defect sites increase, and then the corresponding exciton capture centre increases, and accordingly, the QY of CDs will rise.30
| CDs | C 1s | O 1s | |||
|---|---|---|---|---|---|
C C/% |
C–C/% | C O/% |
C O/% |
C–OH/% | |
| TA-CDs | 18.07 | 79.82 | 2.11 | 40.85 | 59.15 |
| MA-CDs | 12.25 | 84.82 | 2.93 | 47.67 | 52.33 |
| LA-CDs | 13.23 | 83.02 | 3.75 | 51.36 | 48.64 |
| OA-CDs | 24.49 | 71.84 | 3.68 | 52.02 | 47.98 |
| a-CDs | 16.55 | 79.61 | 3.84 | 56.22 | 43.78 |
| CA-CDs | 20.50 | 73.71 | 5.79 | 61.24 | 38.76 |
C bonds, respectively.19 CDs all exhibit the absorption peaks centred at 320–360 nm attributed to the n–π* transition of C
O bonds.31 CA-CDs and a-CDs have high QY values, and their corresponding UV-vis absorption peaks at 360 nm are strong, which qualitatively indicates that the contents of C
O are high.31 The other four CDs with low QY exhibit weak and similar absorption peak at around 325 nm. This is consistent with the analysis results of XPS, further confirming that the high content of C
O could promote the synthesis of CDs with high QY. These absorption changes disclose that the surface states of CDs have been changed through changing the contents of O-containing precursors, which significantly affects the photoluminescence performance of CDs.29As an important optical property of CDs, the fluorescence emission spectra of CDs from different carbon sources under various excitation wavelengths are shown in Fig. 2a–f. By comparison, it can be seen that TA-, MA-, LA- and OA-CDs with low QY have a similar feature of excitation-wavelength dependence. The excitation-wavelength dependence may be derived from the heterogeneous size of TA-, MA-, LA- and OA- or diverse surface states.15 Meanwhile, CA-CDs and a-CDs with high QY have the property of excitation-wavelength independence, which reflects that the surface states of CA-CDs and a-CDs are originated from a single energy level, and almost all of excited electrons can return to the ground state through the radiation route. Therefore, the passivation degree of the trap on the surface of CA-CDs and a-CDs is enhanced, leading to the increase of the fluorescence QY of CA-CDs and a-CDs.32
In order to further analyse the fluorescence properties and their origins of CDs from different carbon sources, the fluorescence lifetimes of CDs were measured. The PL decay curves of CDs except a-CDs fit with a double-exponential function and provide PL lifetimes in the range of 9.46–14.62 ns. The PL decay curve of a-CDs fits with a single-exponential function and their lifetime is 18.00 ns (Fig. 2g). The corresponding fitting parameters are as shown in Table S4.† α1 refers to the proportion of short lifetime τ1 deriving from carbon nuclear state, and α2 refers to the proportion of long lifetime τ2 deriving from surface state. Therefore, the QY of CDs mainly benefits from the contribution of surface states. Fig. 2g illustrates that from top to bottom, the QY of CDs gradually increases, and in the meantime the decay rate of τ is gradually slows down. As a whole, with the increase of the QY values of CDs, the values of long lifetime τ2 gradually increased, and fluorescence lifetime showed a trend of gradual increase (Table S4†). The increase of fluorescence lifetime may be attributed to the decrease of the non-radiation traps or the increase of emission sites resulting from surface passivation of CDs.33 Meanwhile, the change trend of lifetime of CDs is consistent with that of the content of C
O bond, which shows the O-containing functional groups on the surface of CDs have great contribution to the QY.
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| Fig. 3 Schematic structure of CDs synthesized with different carbon sources: (a) TA-CDs, (b) MA-CDs, (c) LA-CDs, (d) OA-CDs, (e) a-CDs and (f) CA-CDs, silane coupling agent is KH-792. | ||
Moreover, the PY values of CDs from different carbon sources were high and similar, from 52.56% to 58.76%, this is because the carboxyl and hydroxyl groups from carbon sources and amine and siloxane groups from KH-792 can undergo dehydration, condensation and crosslinking reactions, and the crosslinking structure benefits for the high PY of CDs,22,23 and the degree of cross-linking reaction between different carbon sources and silane coupling agents may be similar.
To sum up, it was found that the fluorescence of CDs from different carbon sources mainly comes from surface state luminescence rather than the quantum size effect. The influence mechanism of O-containing functional groups on CDs is presented, as shown in Fig. 4. The QY values of CDs synthesized using different carbon sources are closely related to the O-containing functional groups on the surface of carbon sources, specifically, the higher the content of C
O, the higher the QY value of CDs. The PY value of CDs depends on whether CDs has the crosslinking structure.
Consequently, it is found that the QY values of CDs synthesized using different silane coupling agents is closely related to the content of amino groups, and the PY values of CDs still depends on whether the reactants can undergo crosslinking reaction. The main text of the article should appear here with headings as appropriate.
The FTIR spectra of CDs from different silane coupling agents are as shown in Fig. 5d. The typical bands at 1030 and 1124 cm−1 originating from the stretching vibration of Si–O–Si, the absorption peak at 1657 cm−1 arises from –CONH– bond and the broad band within 3050–3650 cm−1 deriving from the stretching vibrations of O–H and N–H,17 which represent CA all has reacted with different silane coupling agents.20,29 The intensity of Si–O–Si, N–H and C
O peaks (relative to that of CONH) of CA-CDs are the highest, and the O–H band of CA-CDs are the widest, which further manifests that KH-792 has the highest degree of hydrolysis in the presence of CA and the reaction between CA and KH-792 are most complete, which leads to the highest QY of CA-CDs. Also, it has been proved that high N- and O-containing functional groups boost the QY of CDs.
The results of element analysis in Table S6† and the XPS spectra of CDs in Fig. S5† show that all CDs from different silane coupling agents are mainly composed of C, O and N with tiny amount of Si, and CA-CDs have the highest content of O. According to the element content analysis results of XPS (Table S7†), the element contents of CDs are of significant difference, because of the different contents of methoxy and amino groups on the surface of different silane coupling agents. These elements further influence the QY of CDs from different silane coupling agents, which is consistent with the results of CDs from different agents, which is consistent with the results of CDs from different carbon sources.
Fine scan XPS spectra of C 1s and O 1s for the CDs from different silane coupling agents are given in Fig. 5e, and the percentage composition of each bond has quantificationally analysed as shown in Table 2. The C 1s spectrum indicates C mainly exists in forms of C–C/C
C, C–N/C–O and C
O. The N 1s spectra of CDs can validate the existence of pyridinic N, amino N and pyrrolic N.
| CDs | C 1s | N 1s | ||||
|---|---|---|---|---|---|---|
C–C/C C/% |
C–N/C–O/% | C O/% |
Pyridinic N/% | Amino N/% | Pyrrolic N/% | |
| 540-CDs | 75.36 | 19.89 | 4.75 | 60.43 | 36.12 | 3.45 |
| 602-CDs | 70.11 | 24.02 | 5.86 | 73.52 | 20.23 | 6.25 |
| CA-CDs | 64.03 | 29.53 | 6.44 | 63.82 | 27.37 | 8.81 |
With the peak intensity and the percentage composition of C
O and pyrrolic N separately on the surface of CDs gradually increased, the QY values of 540-, 602- and CA-CDs in Table S5† correspondingly increases. This proves that the content of C
O and pyrrolic N both have a positive effect on the QY of CDs from different silane coupling agents. The PY values of 540-, 602- and CA-CDs increase with the increasing amount of pyridinic N and the decreasing amount of amino N. This can indicate the high content of pyridinic N and low content of amino N contributes to the high PY of CDs from different silane coupling agents.
O bonds. The QY values of 602-CDs and CA-CDs are high and the corresponding absorption peaks at 360 nm are strong, which qualitatively shows the high content of C
O.31 This is compatible with XPS results, indicating that high content of C
O is beneficial for the high QY of CDs.27 It is can be seen that from the Fig. 6, 540-CDs with lowest QY value shows excitation wavelength-dependent property, whose fluorescent intensity is lower than the other two by comparison. On the contrary, the other two CDs with higher QY have the excitation wavelength-independent property. This result is consistent with the results of CDs from different carbon sources.
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| Fig. 6 (a–c) Fluorescence emission spectroscopy and (d) fluorescence decay curve of CDs synthesized with different silane coupling agents (carbon source is CA). | ||
The fluorescence lifetimes of CDs from different silane coupling agents are presented in Fig. 6d and the corresponding parameters are shown in Table S8.† The decay curve of CA-CDs can be well fitted by a double exponential function and while the other two CDs can be fitted by a single exponential function. The slower the decay rate of lifetime, the higher the QY of CDs. Table S8† indicates the longer the lifetime of CDs, the higher the QY. It demonstrates the fluorescence of CDs from different silane coupling agents mainly derives from the surface state. Consequently, QY of CDs is mainly attributed to their surface structure.
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| Fig. 7 Schematic structure of CDs synthesized with different silane coupling agents: (a) 540-CDs, (b) 602-CDs and (c) CA-CDs, carbon source is CA. | ||
The difference in QY and PY of CDs from different silane coupling agents should not originate from the quantum size effect but surface state. Silane coupling agent contains different number of methoxy and amino groups, and different chain lengths, so the QY and PY values of corresponding synthesized CDs are different. KH-602 has one less methoxy group than KH-792, so the QY value of 602-CDs is slightly lower than that of CA-CDs, while KH-540 has a shorter chain length and one less amino group than KH-792, so the QY value of 540-CDs is much lower than that of CA-CDs, indicating amino groups have a significant effect on QY of CDs and methoxy group have little influence on QY of CDs. Specifically, the content of C
O and pyrrolic N both have a positive effect on the QY of CDs. Therefore, the organosilane functional groups including O- and N-containing functional groups make a significant contribution to high QY of CDs. It is because that on one hand, in the hydrothermal process, the amino group on the side chain of the silane coupling agent can react with the carboxyl group of CA to form an amide bond; on the other hand, each silane coupling agent contains two or three methoxy groups, after hydrolysis, they will form silanol groups which are highly reactive intermediates responsible for condensation with other silanes and hydroxyl groups from CA.36
Moreover, the PY values of 540-, 602- and CA-CDs were high and similar, from 46.33% to 58.53%, further verifying CDs with the crosslinked structure contributing to high PY, which is consistent with the results of CDs from different carbon sources. Meanwhile, it is also found that high content of pyridinic N and low content of amino N favour for the high PY of CDs from different silane coupling agents.
In summary, the fluorescence of CDs from different silane coupling agents mainly depends on surface state luminescence not quantum size effect. The synergistic influence mechanism of O- and N- containing functional groups on CDs is presented, as shown in Fig. 8. The high content of C
O and pyrrolic N boost the QY enhancement of CDs. CDs with the property of excitation independence and long lifetime generally have high QY. CDs with the crosslinked structure generally have high PY, and high content of pyridinic N and the low content of amino N are in favor of CDs with high PY.
O bond and pyrrolic N) have a significant synergistic effect on the QY of CDs. CDs with the property of excitation independence and long lifetime generally have high QY. The highest QY of CDs is up to 97.32%. The PY value of CDs is closely related to the crosslink structure of CDs, and positively correlated with the pyridinic N content and negatively correlated with amino N. The PY of CDs is all above 46%. Therefore, the selection of raw materials rich in carboxyl groups and amino groups is conducive to the synthesis of high QY of CDs, and high content of pyrrolic N on CDs surface can enhance the QY. Furthermore, whether the reactants can undergo crosslink reaction also contributes to the PY values of CDs and high content of pyridinic N is favourable for preparing high PY of CDs. The above results provide theoretical guidance for synthesizing CDs with high QY on a large scale.
Footnote |
| † Electronic supplementary information (ESI) available. See https://doi.org/10.1039/d2ra05623b |
| This journal is © The Royal Society of Chemistry 2022 |