Wenqian Zhao

In this study, we examined the frequently reported “selective fluorescence quenching effects” of Fe

 ions on carbon dots. Instead of the believed “quenching effects” by Fe

, the strong reduction of the fluorescence of carbon dots is likely because of the inner filter effect, which is caused by the strong ultraviolet (UV) absorption of Fe With the addition of Fe

 ions, the UV absorption increases dramatically, compared to other metal ions. When Fe

 ions coexist with carbon dots (CDs) in the solution, most of the excitation light is absorbed by Fe

 ions, decreasing the excitation light obtained by CDs. This phenomenon leads to the “fluorescence quenching.” This finding helps us gain a better understanding of the fluorescence quenching effects of metal ions on carbon dots and understand the quenching effect of metal ions on other fluorescent materials.

Heavy metal ions are critically important to certain biological functions, but they are also considered environmentally hazardous and detrimental to human health if not handled and treated with the necessary precautions (1–7). As a result, methods of identification and quantification are necessary. Carbon dots (CDs) have attracted considerable attention as photocatalysts (8), sensors (9–10), printing inks (11), in drug delivery (12), and in bioimaging materials (13), because of their unique optical, electronic, and chemical properties. Because of the unique properties of CDs, metal ions demonstrate different fluorescence quenching effects on them. Particularly, Cu

ions have special fluorescence quenching effects on CDs, as summarized in Table I (14–24). However, there are still some important questions that need to be addressed. Why can Fe

 ions selectively quench many types of carbon dots? And why is there no wide range of linear relationships between the quenching effects and the Fe

 concentration, especially at relatively high concentrations (CFe

As shown in Table I, regardless of the raw materials, the preparation methods of CDs or the ion quenching conditions used, Fe

 ions have special selective fluorescence quenching effects on nearly all CDs. The selective fluorescence quenching of CDs by metal ions is because of the strong binding energy between the ions and the electron-rich nitrogen and oxygen groups on the surface of CDs (2,4–5,7,9–10). This theory can explain most cases; however, when it comes to Fe

For example, when it comes to electron capacity, which occurs in the order:

 is stronger than that of others, the fluorescence quenching effect of Ag

(17–18,23,25). This observation conflicts with the general assumption that electron capacity order determines quenching effect order. Furthermore, the ability of the Hg

 ion to obtain electrons is stronger than that of the Fe

 ion; however, in most cases, the fluorescence quenching effect of the Hg

 ion is also much lower than that of the Fe

 ion, which is also in conflict with the current general assumption.

In this study, we attempted to obtain a valid explanation for the selective fluorescence quenching effects on CDs.

All chemicals used were of analytical reagent grade, except garlic and grass samples. The compounds lithium chloride (LiCl), sodium chloride (NaCl), sodium hydroxide (NaOH), potassium chloride (KCl), silver nitrate (AgNO3), mercury (II) chloride (HgCl

), were purchased from Sinopharm Chemical Reagent Co., Ltd. The stock solutions of metal salts were prepared using distilled water.

To confirm and further investigate the quenching mechanism in Table I, four kinds of CDs, namely CD-A, CD-B, CD-C, and CD-D, were made from different raw materials such as grass, glycine, glucose, citric acid, ethylenediamine, and garlic, according to previous studies (18–20,25).

The ultraviolet-visible (UV-vis) absorption spectrum was obtained with a Cary 60 UV-vis spectrophotometer (Agilent Technologies). The photoluminescence (PL) spectra of CDs were obtained with a Cary Eclipse fluorescence spectrophotometer (Varian).

The QY of CDs was measured according to an established procedure (26). Quinine sulfate in 0.1 M of H

 (the literature QY is 0.54 at 360 nm) was chosen as a standard. Absolute values were calculated using the standard reference sample that had a fixed and known fluorescence QY value. To minimize the absorption effects, the absorbance in the 10 mm fluorescence cuvette were kept under 0.1 at the excitation wavelength (360 nm). The QY was estimated to be 6.8%, 4.2%, 4.6%, and 7.3% for CD-A, CD-B, CD-C, and CD-D, respectively.

The experiment was performed at room temperature in distilled water. In a typical run, CD dispersion was diluted with distilled water to make sure the UV absorbance was lower than 0.1. The metal ions were also prepared in aqueous solution with distilled water. Subsequently, 10 mL of the as-prepared CD solution and 10 mL of the metal ion solution was mixed in a 25 mL glass bottle. The PL spectra were recorded after reaction for 5 min at room temperature.

Figure 3 demonstrates that the CD-C material in aqueous solution has a single UV-vis absorption peak at 345 nm, and very bright blue luminescence under the illumination of UV (365 nm) light, even at a very low concentration (Absorbance <0.1). The CD-C aqueous solution can be seen in the inset of Figure 1. Excitation-dependent PL behavior was also observed as the literature (18), which is common in some fluorescent carbon materials (Figure 1) (27–30). When the excitation wavelength is changed from 300 nm to 400 nm, the emission wavelength demonstrated hardly any shift. This behavior contributes to the surface state affecting the bandgap of CDs (31). In the fluorescence spectra in Figure 1, CD-C has optimal excitation and emission wavelengths at 345 nm and 440 nm, which are different from the literature (19).

FIGURE 1: Fluorescence emission spectra (slit ex = 2.5 nm, em = 5 nm) and UV-vis absorbance spectra of CD-C; Inset: Photograph of CD-C under the illumination of UV (365 nm) light (left) and white light (right).

FIGURE 3: UV-vis spectra of the metal ions and the quenching samples with CD-C. (a) UV absorbance of 1 mM metal ions. (b) UV absorbance of the quenching samples with 1 mM metal ions. (c) UV absorbance of quenching samples with different concentrations of Fe

 concentration (0.005–1.000 mM) and the increased absorbance of the samples at 345 nm.

We investigated the fluorescence quenching effects of various metal ions on CDs in distilled water (Figure 2). A series of metal ions (Li

), each at a concentration of 1 mM were used in the experiment. As shown in Figure 2, the fluorescence quenching effects of the Fe

 ions were much stronger than that of the other ions for all four of the synthesized CDs. According to previous work, there must be a unique mechanism that has yet to be accounted for.

FIGURE 2: Fluorescence quenching effects of 1 mM metal ions on CDs in distilled water corresponding to (a) CD-A, (b) CD-B, (c) CD-C, and (d) CD-D, respectively (ex = 345 nm, em = 440 nm).

Subsequent experimentations revealed that the selective quenching effects of Fe

 on CDs were likely caused because of the inner filter effect, which occurred because of the strong UV absorbance of the Fe

 ions (Figure 3a). When the CDs solution was mixed with Fe

, the UV absorbance of the samples would dramatically increase compared to other metal ions (Figure 3b). To investigate the Fe

 fluorescence quenching effects on CDs, CD-C was used in the quenching experiments because of its high QY.

, 1 mM) and their corresponding quenching samples are demonstrated in Figure 3. Figure 3a shows the UV absorbance of the metal ions aqueous solutions; apparently, only Fe

 solutions have strong UV absorbance, whereas the other metal ions have hardly any absorption. As shown in Figure 3b, the addition of the Fe

ions would greatly enhance the UV absorption of the samples compared to the original CD solution. The absorbance of the samples intensified as the concentration of Fe

 ions increased (Figure 3c). The increased absorbance is as high as 0.81 (1 mM Fe

, 345 nm), and the excitation light could likely be absorbed by Fe

 ions to some extent, decreasing the excitation light obtained by CDs and contributing to the quenching effects.

Finally, Figure 3d shows there is a highly correlated linear relationship between the Fe

 concentration and the increased absorbance of the samples at 345 nm (which is the optimal excitation wavelength of CD-C). This indicates that it is possible to detect Fe

 by UV absorbance when using CDs as sensors. In comparison, there is no good linear relationship between Fe

 concentration and its absorbance (Figure 4b).

 ions “quenching effects” on CD-C in distilled water. (ex = 345 nm, em = 440 nm, slit ex = 2.5 nm, em = 5 nm). (a) “FL quenching” spectra of CD-C with different concentrations of Fe

. (b) Relationship between the “quenching effects” and the increased absorbance at 345 nm and the relationship between the “quenching effects” and the Fe

 ions in the samples absorb the excitation light and cause a decrease of the fluorescence intensity of the samples.

As shown in Figure 4a, only minor “quenching effects” were observed when the concentration of Fe

 M. This observation demonstrates that there is hardly any UV absorbance below concentration of 10

 M (as shown in Figure 3c). We observe that the correlation between the “fluorescence quenching effects” and the increased absorbance (due to the Fe

 concentration) is not linear. This phenomenon also has been found in other cases especially when the Fe

 M (14,18). These nonlinear relationships indicate that the inner filter effect may be the main factor causing the “quenching effects,” but that it may not be the only factor. They can be functionalized via an exponential decay model with 

-squared values of 0.99887 and 0.99944, respectively (Table II).

To further investigate the connections between the increased absorbance and the “quenching effects” on CDs, we conducted quenching experiments at different excitation wavelengths with CD-C. Under this circumstance, the absorbance of the samples would change along with the excitation wavelength, whereas the concentration of Fe

 would remain unchanged. As shown in Figure 5, the “quenching effects” decreased as the absorbance became weaker. This correlation is similar to that demonstrated in Figure 4b, with the correlation between fluorescence “quenching effects” and the absorbance also fitting very well with an exponential decay model demonstrating an 

FIGURE 5: Correlations between fluorescence “quenching effects” and the increased UV absorbance of the samples at different excitation wavelengths. (0.5 mM Fe

, distilled water, em = 440 nm, ex = 300–400 nm, 10 nm interval, slit ex = 2.5 nm, em = 5 nm).

CD solutions demonstrate on–off fluorescence phenomena with oxidation-reduction reactions with Fe

 ions (19,32), this could be because the absorbance of the samples with Fe

 ions (Figure 3b). Therefore, the selective “quenching effects” of Fe

 on CDs are likely because of the strong UV absorbance of the Fe

 ions also have selective quenching effects on other fluorescent materials like metal-organic frameworks (MOFs) (33–37), rare earth materials (38), and organic chemosensors (39). The correlations between the quenching effects and the Fe

 concentrations showed the similar pattern (nonlinear when the Fe

 M). Based on the above observations, the selective quenching effects on these materials may also be because of the inner filter effect caused by the strong UV absorption of Fe

This report demonstrates the main reason why Fe

 ions have selective quenching effects on CDs. The finding that the strong UV absorption of Fe

 ions at specific concentrations plays a key role in the fluorescence quenching effects on carbon dots may help us to gain a better understanding of the quenching mechanisms and promote the application development of fluorescent metal ions sensors.

This work was supported by the China Scholarship Council (No.201808410585) for overseas research. We also appreciate the support from the School of Biological and Chemical Sciences, University of Missouri–Kansas City.

(1) S. Liu, J.Q. Tian, L. Wang, Y.W. Zhang, X.Y. Qin, Y.I. Luo, A.M. Asiri, A.O. Al-Youbi, and X.P. Sun, 

(2) Z.X. Qin, W.H. Wang, X.Z. Zhan, X.J. Du, Q.M. Zhang, R. Zhang, K. Li, J.H. Li, and W.P. Xu, 

(3) J.F. Shangguan, J. Huang, D.G. He, X.X. He, K. Wang, R.Z. Ye, X. Yang, T.P. Qing, and J. L. Tang, 

(4) B.S. Chen, F.M. Li, L.L. Zou, D.J. Chen, 

(5) X. Zhu, J.Y. Wang, Y.H. Zhu, H.H. Jiang, D. Tan, Z.Q. Xu, T. Mei, J.H. Li, L.J. Xue, and X.B. Wang, 

(6) K. Karali, L. Sygellou, and C. Stalikas, 

(7) J.H. He, Y.Y. Cheng, T. Yang, H.Y. Zou, and C.Z. Huang, 

(8) H.T. Li, X.D. He, Z.H. Kang, H. Huang, Y. Liu, J.L. Liu, S.Y. Lian, C.H.A. Tsang, X.B. Yang, and S.T. Lee, 

(9) X.H. Gao, Y.Z. Lu, R.Z. Zhang, S.J. He, J. Ju, M.M. Liu, L. Li, and W. Chen, 

(10) J. Plácido, S. Bustamante-López, K. E. Meissner, D. E. Kelly, and S. L. Kelly, 

(11) R.Q. Bao, Z.Y. Chen, Z.W. Zhao, X. Sun, J.Y. Zhang, L.R. Hou, and C.Z. Yuan, 

(12) Q.L. Wang, X.X. Huang, Y.J. Long, X.L. Wang, H.J. Zhang, R. Zhu, L.P. Liang, P. Teng, and H.Z. Zheng, 

(13) L. Cao, X. Wang, M.J. Meziani, F.S. Lu, H.F. Wang, P.G. Luo, Y. Lin, B.A. Harruff, L.M. Veca, D. Murray, S.Y. Xie, and Y.P. Sun, 

(14) L.Q. Liu, Y.F. Li, L. Zhan, Y. Liu, and C.Z. Huang, 

(15) L. Zhou, Y.H. Lin, Z.Z. Huang, J.S. Ren, and Q.X. Gang, 

(16) C.Y. Wang, C.F. Wang, P.P. Xu, A.Q. Li, Y.J. Chen, and K.L. Zhuo, 

(17) S. Liu, J.Q. Tian, L. Wang, Y. Zhang, X. Qin, Y. Luo, A.M. Asiri, A.O. Al-Youbi, and S.X. Qing, 

(18) T.T. Lai, E.H. Zheng, L.X. Chen, X.Y. Wang, L.C. Kong, C.P. You, Y.M. Ruan, and X.X. Weng, 

(19) S.J. Zhu, Q.N. Meng, L. Wang, J.H. Zhang, Y.B. Song, H. Jin, K. Zhang, H.C. Sun, H. Y. Wang, and B. Yang, 

(20) M. Zhou, Z.L. Zhou, A.H. Gong, Y. Zhang, Q.J. Li, 

(21) Q. Xu, P. Pu, J.G. Zhao, C.B. Dong, C. Gao, Y.S. Chen, J.R. Chen, Y. Liu, H.J. Zhou, 

(22) T.N.J.I. Edison, R. Atchudan, J.J. Shim, S. Kalimuthu, B.C. Ahn, and Y.R. Lee, 

(23) R.L. Liu, M.P. Gao, J. Zhang, Z.L. Li, J.Y. Chen, P. Liu, D. Q. Wu, 

(24) Y.F. Chen, Y.Y. Wu, B. Weng, B. Wang, C.M. Li, 

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(26) F. Wang, Z. Xie, H. Zhang, C.Y. Liu, and Y.G. Zhang, 

(27) R.L. Liu, D.Q. Wu, S.H. Liu, K. Koynov, W. Knoll, and Q. Li, 

(28) M.J. Krysmann, A. Kelarakis, P. Dallas, and E.P. Giannelis, 

(30) X.Y. Zhai, P. Zhang, C.J. Liu, T. Bai, W.C. Li, L.M. Dai, and W. G. Liu, 

(31) D.Y. Pan, J.C. Zhang, Z. Li, C. Wu, X.M. Yan, and M.H. Wu, 

(32) X. Miao, Y.X. Long, D. Qu, D.B. Li, F.F. Tao, Z.C. Sun, 

(33) X.-H. Zhou, L. Li, H.-H. Li, A. Li, T. Yang, W. Huang, 

(34) C. Zhang, Y. Yan, Q.H. Pan, L. Sun, H.M. He, Y.L. Liu, Z.Q. Liang, and J.Y. Li, 

(35) Y.F. Li, D. Wang, Z. Liao, Y. Kang, W.H. Ding, X.J. Zheng, and L.P. Jin, 

(36) B. Wang, Q. Yang, C. Guo, Y.X. Sun, L.H. Xie, J.R. Li, 

(37) Y.T. Yan, J. Liu, G.P. Yang, F. Zhang, Y.K. Fan, W.Y. Zhang, Y. Y. Wang, 

(38) L.M. Zhang, B. Li, S.Z. Min, and S.M. Yue, 

(39) X.D. Yang, X.L. Chen, X.D. Lu, C.G. Yan, Y.K. Xu, X.D. Hang, J.Q. Qu, and R.Y. Liu, 

 is with the School of Chemistry and Pharmaceutical Engineering at Huanghuai University in Zhumadian, China, and the Department of Chemistry, at the University of Missouri–Kansas City, in Kansas City, Missouri. 

 are with the School of Chemistry and Pharmaceutical Engineering at Huanghuai University in Zhumadian, China. 

 are with the Department of Chemistry, at the University of Missouri–Kansas City, in Kansas City, Missouri. 

 is with Green Intelligence Environmental School at Yangtze Normal University in Chongqing, China. Direct correspondence to: 

Articles

The “selective fluorescence quenching effects” of Fe3+ ions on carbon dots are examined to gain a more comprehensive understanding of the interactions of metal ions with a variety of fluorescent materials.

Wenqian Zhao

Articles

Fluorescence Quenching Effects of Fe3+ Ions on Carbon Dots