Ternary Composite of Co-Doped CdSe@electrospun Carbon Nanoﬁbers: A Novel Reusable Visible Light-Driven Photocatalyst with Enhanced Performance

: In this work, ﬂexible ternary composites of cobalt-doped cadmium selenide / electrospun carbon nanoﬁbers (Co-CdSe@ECNFs) for photocatalytic applications were fabricated successfully via electrospinning, followed by carbonization. For the fabrication of the proposed photocatalysts, Co-CdSe nanoparticles were grown in situ on the surface of ECNFs during the carbonization of precursor electrospun nanoﬁbers obtained by dispersing Se powder in the electrospinning solution of polyacrylonitrile / N,N -Dimethylformamide (PAN / DMF) containing Cd 2 + and Co 2 + . The photocatalytic performance of synthesized samples is investigated in the photodegradation of methylene blue (MB) and rhodamine B (RhB) dyes. Experimental results revealed the superior photocatalytic e ﬃ ciency of Co-CdSe@ECNFs over undoped samples (CdSe@ECNFs) due to the doping e ﬀ ect of cobalt, which is able to capture the photogenerated electrons to prevent electron–hole recombination, thereby improving photocatalytic performance. Moreover, ECNFs could play an important role in enhancing electron transfer and optical absorption of the photocatalyst. This type of fabrication strategy may be a new avenue for the synthesis of other ECNF-based ternary composites.


Introduction
Contamination of bodies of water such as ground water, lakes, rivers, and seas with toxic chemicals or foreign substances caused by improper disposal of waste water from different industrial plants has become a global challenge, as these contaminants have adverse effects on human and aquatic life. However, while industrialization is the key initiator of development and urbanization of a society, it has been recognized as a major cause of water pollution. The effluents discharged from industrial plants contain a number of toxic pollutants ranging from organochloride-based pesticides to heavy-metal-associated non-biodegradable organic dyes, which cause the contamination of natural water sources and subsequent health problems [1]. Different attempts, comprising biological treatment, adsorption by activated carbon, reverse osmosis, coagulation, and ion exchange, have been made to address the issue of water contamination, however, none of these conventional water treatment Figure 1 illustrates the X-ray diffraction (XRD) patterns of ECNFs, CdSe@ECNFs, and Co-CdSe@ECNFs. The characteristic peaks displayed by CdSe@ECNFs and Co-CdSe@ECNFs at 2θ of 25.24 • , 42.2 • , and 49.9 • corresponding to the crystallographic planes (111), (220), and (311) were associated with the cubic CdSe phase (JCPDS: 65-2891). The peak displayed by all samples at 2θ of 22.5 • was associated with the (002) crystallographic plane of graphitic carbon. However, none of the characteristic peaks of Co and its compound impurity were detected in the XRD pattern of Co-CdSe@ECNFs, which might be attributed to the substitution of Cd 2+ by Co 2+ from the CdSe crystal lattice due to the smaller radius of Co 2+ (0.75 Å) compared to that of Cd 2+ (0.95 Å). Therefore, Co 2+ could be easily inserted into the CdSe crystal lattice, rather than forming a mixture [39].

Results and Discussion
Catalysts 2020, 10, 348 3 of 15 CdSe@ECNFs might be an ideal strategy to obtain a ternary composite as an efficient photocatalyst.
To the best of our knowledge, this type of work has not been reported so far. Figure 1 illustrates the X-ray diffraction (XRD) patterns of ECNFs, CdSe@ECNFs, and Co-CdSe@ECNFs. The characteristic peaks displayed by CdSe@ECNFs and Co-CdSe@ECNFs at 2θ of 25.24°, 42.2°, and 49.9° corresponding to the crystallographic planes (111), (220), and (311) were associated with the cubic CdSe phase (JCPDS: 65-2891). The peak displayed by all samples at 2θ of 22.5° was associated with the (002) crystallographic plane of graphitic carbon. However, none of the characteristic peaks of Co and its compound impurity were detected in the XRD pattern of Co-CdSe@ECNFs, which might be attributed to the substitution of Cd 2+ by Co 2+ from the CdSe crystal lattice due to the smaller radius of Co 2+ (0.75 Å) compared to that of Cd 2+ (0.95 Å). Therefore, Co 2+ could be easily inserted into the CdSe crystal lattice, rather than forming a mixture [39]. The morphology and elemental composition of different samples are presented in field emission scanning electron microscopy (FESEM) images ( Figure 2). Figure 2a shows a typical FESEM image of ECNFs. As can be seen, ECNFs were uniform, continuous, randomly oriented, and possessed smooth surfaces without secondary nanostructures. In comparison with ECNFs, no apparent change was observed in the overall pattern of CdSe@ECNFs ( Figure 2b) and Co-CdSe@ECNFs ( Figure 2c). However, the surface of the carbon nanofibers was no longer smooth. The high-magnification images (insets of Figure 2b,c) reveal that the surfaces of the ECNFs were coarse due to the growth of numerous nanoparticles after carbonization. The nanoparticles were uniformly distributed across the surface of each carbon nanofiber without aggregation, thereby offering a high surface area for the nanoparticles. Figure 2d represents the energy dispersive X-ray spectroscopy (EDS) spectrum along with wt% of elements (inset) of Co-CdSe@ECNFs. As shown in the spectrum, the existence of considerable amounts of C, Co, Cd, and Se elements could confirm the doping of Co in CdSe nanoparticles supported on ECNFs. The inset in Figure 2a is a digital photograph of a flexible nanofibrous mat of Co-CdSe@ECNFs. Moreover, the elemental mapping images of Co-CdSe@ECNFs ( Figure 3) reveal the uniform distribution of Co, Cd, and Se elements on the surface of carbon nanofibers, signifying the successful fabrication of the ternary composite. The morphology and elemental composition of different samples are presented in field emission scanning electron microscopy (FESEM) images ( Figure 2). Figure 2a shows a typical FESEM image of ECNFs. As can be seen, ECNFs were uniform, continuous, randomly oriented, and possessed smooth surfaces without secondary nanostructures. In comparison with ECNFs, no apparent change was observed in the overall pattern of CdSe@ECNFs ( Figure 2b) and Co-CdSe@ECNFs ( Figure 2c). However, the surface of the carbon nanofibers was no longer smooth. The high-magnification images (insets of Figure 2b,c) reveal that the surfaces of the ECNFs were coarse due to the growth of numerous nanoparticles after carbonization. The nanoparticles were uniformly distributed across the surface of each carbon nanofiber without aggregation, thereby offering a high surface area for the nanoparticles. Figure 2d represents the energy dispersive X-ray spectroscopy (EDS) spectrum along with wt% of elements (inset) of Co-CdSe@ECNFs. As shown in the spectrum, the existence of considerable amounts of C, Co, Cd, and Se elements could confirm the doping of Co in CdSe nanoparticles supported on ECNFs. The inset in Figure 2a is a digital photograph of a flexible nanofibrous mat of Co-CdSe@ECNFs. Moreover, the elemental mapping images of Co-CdSe@ECNFs ( Figure 3) reveal the uniform distribution of Co, Cd, and Se elements on the surface of carbon nanofibers, signifying the successful fabrication of the ternary composite.  In order to observe the fiber morphology and degree of dispersion of nanoparticles on the surface of ECNFs, transmission electron microscopy (TEM) analysis was performed ( Figure 4). Figure  4a shows a TEM image of an ECNF with a nanofibrous morphology possessing a relatively smooth surface. In comparison, the surface of Co-CdSe@ECNFs were somewhat rough due to the growth of numerous Co-CdSe nanoparticles on the surface of the ECNFs, as described in the FESEM analysis. The nanoparticles having an average size of 9 nm grew uniformly on the surface of ECNFs, as shown in the high-magnification TEM image (Figure 4c) obtained from the red circled area of Figure 4b. More interestingly, the sonication process during sample preparation for the TEM analysis did not cause nanoparticles to fall off the ECNFs, which signified the strong attachment between nanoparticles and the ECNF surface. The perfectly crystalline structure of Co-CdSe nanoparticles was observed by high resolution-TEM (HR-TEM) (Figure 4d), recorded from the blue circled area of   In order to observe the fiber morphology and degree of dispersion of nanoparticles on the surface of ECNFs, transmission electron microscopy (TEM) analysis was performed ( Figure 4). Figure  4a shows a TEM image of an ECNF with a nanofibrous morphology possessing a relatively smooth surface. In comparison, the surface of Co-CdSe@ECNFs were somewhat rough due to the growth of numerous Co-CdSe nanoparticles on the surface of the ECNFs, as described in the FESEM analysis. The nanoparticles having an average size of 9 nm grew uniformly on the surface of ECNFs, as shown in the high-magnification TEM image (Figure 4c) obtained from the red circled area of Figure 4b. More interestingly, the sonication process during sample preparation for the TEM analysis did not cause nanoparticles to fall off the ECNFs, which signified the strong attachment between nanoparticles and the ECNF surface. The perfectly crystalline structure of Co-CdSe nanoparticles was observed by high resolution-TEM (HR-TEM) (Figure 4d), recorded from the blue circled area of In order to observe the fiber morphology and degree of dispersion of nanoparticles on the surface of ECNFs, transmission electron microscopy (TEM) analysis was performed ( Figure 4). Figure 4a shows a TEM image of an ECNF with a nanofibrous morphology possessing a relatively smooth surface. In comparison, the surface of Co-CdSe@ECNFs were somewhat rough due to the growth of numerous Co-CdSe nanoparticles on the surface of the ECNFs, as described in the FESEM analysis. The nanoparticles having an average size of 9 nm grew uniformly on the surface of ECNFs, as shown in the high-magnification TEM image (Figure 4c) obtained from the red circled area of Figure 4b. More interestingly, the sonication process during sample preparation for the TEM analysis did not cause nanoparticles to fall off the ECNFs, which signified the strong attachment between nanoparticles and the ECNF surface. The perfectly crystalline structure of Co-CdSe nanoparticles was observed by high resolution-TEM (HR-TEM) (Figure 4d), recorded from the blue circled area of Figure 4c. As can be seen, the inner planar spacing of 0.367 nm, corresponding to the (111) crystallographic plane of CdSe (JCPDS: 65-2891), was clearly observed, revealing its excellent crystallinity. Furthermore, the heterojunction showed that the Co-CdSe nanoparticles attached to the surface of ECNFs had disordered stacking features, indicating its low crystallinity. Additionally, line EDS analysis of the sample was performed at randomly selected points on the line ( Figure 5). As shown in the figure, C, Co, Cd, and Se were detected along the chosen line without any other elemental impurities. Hence, with these characterizations one can claim that the synthesized sample is purely made of C, Co, Cd, and Se, forming a ternary composite of Co-CdSe@ECNFs.

Results and Discussion
Catalysts 2020, 10, 348 5 of 15 Figure 4c. As can be seen, the inner planar spacing of 0.367 nm, corresponding to the (111) crystallographic plane of CdSe (JCPDS: 65-2891), was clearly observed, revealing its excellent crystallinity. Furthermore, the heterojunction showed that the Co-CdSe nanoparticles attached to the surface of ECNFs had disordered stacking features, indicating its low crystallinity. Additionally, line EDS analysis of the sample was performed at randomly selected points on the line ( Figure 5). As shown in the figure, C, Co, Cd, and Se were detected along the chosen line without any other elemental impurities. Hence, with these characterizations one can claim that the synthesized sample is purely made of C, Co, Cd, and Se, forming a ternary composite of Co-CdSe@ECNFs.  The surface element compositions and chemical bonding states of Co-CdSe@ECNFs are presented in the X-ray photoelectron spectroscopy (XPS) results ( Figure 6). The survey spectrum ( Figure 6a) displays corresponding peaks of Co 2p, Cd 4d, Cd 3d, Cd 3p, Se 3d, Se 3s O 1s, and C 1s, indicating the formation of ternary composite. Figure 6b-e shows high-resolution spectra of Co 2p, Cd 3d, Se 3d, and C 1s, respectively. The peaks of Co 2p (Figure 6b) centered at 780.9 eV and 796.7 eV corresponding to Co 2p3/2 and Co 2p1/2, respectively, indicated the existence of Co as Co 2+ [40]. Figure 6c shows a high-resolution spectrum of Cd 3d. The peaks located at 404.6 eV and 411.7 eV were attributed to the Cd 3d5/2 and Cd 3d3/2, respectively. This result confirms the presence of Cd 2+ in Co-CdSe nanoparticles. The high-resolution spectrum of Se ( Figure 6d) showed a peak centered at 54.2 eV, which was assigned to Se 3d [41]. The C 1s XPS spectrum of the sample is shown in Figure  6e. As shown in the figure, a characteristic peak obtained at 284.5 eV was attributed to C-C groups [42]. Thus, XPS analyses indicated the existence of Co 2+ in CdSe crystal lattice forming a ternary composite of Co-CdSe@/ECNFs. In order to elucidate the stability of the photocatalyst, XPS analysis of the utilized sample (Co-CdSe@/ECNFs) was performed and the result is presented in the survey spectrum ( Figure 6f) which displays corresponding peaks of the elements, matching those in Figure  6a. Since no significant change in the chemical composition of these elements was observed, the utilized sample retained its stability. The surface element compositions and chemical bonding states of Co-CdSe@ECNFs are presented in the X-ray photoelectron spectroscopy (XPS) results ( Figure 6). The survey spectrum (Figure 6a) displays corresponding peaks of Co 2p, Cd 4d, Cd 3d, Cd 3p, Se 3d, Se 3s O 1s, and C 1s, indicating the formation of ternary composite. Figure 6b-e shows high-resolution spectra of Co 2p, Cd 3d, Se 3d, and C 1s, respectively. The peaks of Co 2p (Figure 6b) centered at 780.9 eV and 796.7 eV corresponding to Co 2p 3/2 and Co 2p 1/2 , respectively, indicated the existence of Co as Co 2+ [40]. Figure 6c shows a high-resolution spectrum of Cd 3d. The peaks located at 404.6 eV and 411.7 eV were attributed to the Cd 3d 5/2 and Cd 3d 3/2 , respectively. This result confirms the presence of Cd 2+ in Co-CdSe nanoparticles. The high-resolution spectrum of Se ( Figure 6d) showed a peak centered at 54.2 eV, which was assigned to Se 3d [41]. The C 1s XPS spectrum of the sample is shown in Figure 6e. As shown in the figure, a characteristic peak obtained at 284.5 eV was attributed to C-C groups [42]. Thus, XPS analyses indicated the existence of Co 2+ in CdSe crystal lattice forming a ternary composite of Co-CdSe@/ECNFs. In order to elucidate the stability of the photocatalyst, XPS analysis of the utilized sample (Co-CdSe@/ECNFs) was performed and the result is presented in the survey spectrum ( Figure 6f) which displays corresponding peaks of the elements, matching those in Figure 6a. Since no significant change in the chemical composition of these elements was observed, the utilized sample retained its stability. The degree of disorder as well as the composition of different samples are displayed in the Raman spectra in Figure 7. All the samples displayed corresponding peaks at 13,600 cm −1 for D band and 1586 cm −1 for G band. The D and G bands are associated with the sp 3 bonded carbon atoms in disordered carbonaceous matrix and the stretching of sp 2 bonded carbon atoms in graphitic carbon [43,44]. The magnified peaks displayed by the Co-CdSe@ECNFs sample at around 214 cm −1 and 413 cm −1 are assigned as the characteristic peaks of CdSe (inset). Thus, all the information derived from the Raman spectra confirms the formation of composite nanofibers. The degree of disorder as well as the composition of different samples are displayed in the Raman spectra in Figure 7. All the samples displayed corresponding peaks at 13,600 cm −1 for D band and 1586 cm −1 for G band. The D and G bands are associated with the sp 3 bonded carbon atoms in disordered carbonaceous matrix and the stretching of sp 2 bonded carbon atoms in graphitic carbon [43,44]. The magnified peaks displayed by the Co-CdSe@ECNFs sample at around 214 cm −1 and 413 cm −1 are assigned as the characteristic peaks of CdSe (inset). Thus, all the information derived from the Raman spectra confirms the formation of composite nanofibers. Investigation of the photocatalytic activity of a photocatalyst depends upon its light absorption behavior, which plays an important role in determining whether the photocatalyst works under visible light or UV-light. In order to determine this crucial factor UV-Vis diffusive reflectance spectra (DRS) of different samples were measured, and the results are plotted in Figure 8. As shown in Figure  8, ECNFs present the absorption band in visible light and UV-light regions. Meanwhile, it was observed that ECNFs loaded with undoped/Co-doped CdSe nanoparticles displayed obvious visible light absorption behavior, signifying their ability to harvest visible light.  Investigation of the photocatalytic activity of a photocatalyst depends upon its light absorption behavior, which plays an important role in determining whether the photocatalyst works under visible light or UV-light. In order to determine this crucial factor UV-Vis diffusive reflectance spectra (DRS) of different samples were measured, and the results are plotted in Figure 8. As shown in Figure 8, ECNFs present the absorption band in visible light and UV-light regions. Meanwhile, it was observed that ECNFs loaded with undoped/Co-doped CdSe nanoparticles displayed obvious visible light absorption behavior, signifying their ability to harvest visible light. Investigation of the photocatalytic activity of a photocatalyst depends upon its light absorption behavior, which plays an important role in determining whether the photocatalyst works under visible light or UV-light. In order to determine this crucial factor UV-Vis diffusive reflectance spectra (DRS) of different samples were measured, and the results are plotted in Figure 8. As shown in Figure  8, ECNFs present the absorption band in visible light and UV-light regions. Meanwhile, it was observed that ECNFs loaded with undoped/Co-doped CdSe nanoparticles displayed obvious visible light absorption behavior, signifying their ability to harvest visible light. The photocatalytic performances of Co-CdSe@ECNFs and CdSe@ECNFs towards the photodegradation of methylene blue (MB) and rhodamine B (RhB) were evaluated under visible light irradiation. Figure 9a,b shows degradation curves of MB and RhB solutions utilizing different samples along with blank tests. The degradation is represented as the variation of (Ct/Co) with irradiation time, where Co is the initial concentration and Ct is the remaining concentration of the dye solutions at time t. As illustrated in the figures, the blank tests showed negligible degradation of both dye solutions. Similarly, negligible degradation/absorbance of both dye solutions was observed when utilizing ECNFs alone. In contrast, Co-CdSe@ECNFs degraded more than 90% of MB within 70 min, The photocatalytic performances of Co-CdSe@ECNFs and CdSe@ECNFs towards the photodegradation of methylene blue (MB) and rhodamine B (RhB) were evaluated under visible light irradiation. Figure 9a,b shows degradation curves of MB and RhB solutions utilizing different samples along with blank tests. The degradation is represented as the variation of (C t /C o ) with irradiation time, where C o is the initial concentration and C t is the remaining concentration of the dye solutions at time t. As illustrated in the figures, the blank tests showed negligible degradation of both dye solutions. Similarly, negligible degradation/absorbance of both dye solutions was observed when utilizing ECNFs alone. In contrast, Co-CdSe@ECNFs degraded more than 90% of MB within 70 min, while CdSe@ECNFs degraded only 85% of MB within this time. Additionally, the photocatalytic performance of Co-CdSe@ECNFs compared to CdSe@ECNFs for RhB degradation was found to be higher. More than 87% of RhB was degraded within 90 min when utilizing Co-CdSe@ECNFs, but only 81% of RhB was degraded within this time when CdSe@ECNFs was utilized under similar conditions. Based on these results, Co-CdSe@ECNFs was found to be a superior photocatalyst to CdSe@ECNFs for dye degradation under visible light irradiation. The absorbance variation of MB and RhB solutions utilizing Co-CdSe@ECNFs under visible light irradiation at different time intervals is shown in Figure 9c,d. As can be seen, with the increase in irradiation time, all the corresponding absorbance peaks of MB and RhB solutions located at 665 nm and 554 nm were observed to gradually diminish. Furthermore, the color of the corresponding dye solutions gradually weakened with time in the presence of Co-CdSe@ECNFs (insets, Figure 9c,d).
Catalysts 2020, 10, 348 9 of 15 while CdSe@ECNFs degraded only 85% of MB within this time. Additionally, the photocatalytic performance of Co-CdSe@ECNFs compared to CdSe@ECNFs for RhB degradation was found to be higher. More than 87% of RhB was degraded within 90 min when utilizing Co-CdSe@ECNFs, but only 81% of RhB was degraded within this time when CdSe@ECNFs was utilized under similar conditions. Based on these results, Co-CdSe@ECNFs was found to be a superior photocatalyst to CdSe@ECNFs for dye degradation under visible light irradiation. The absorbance variation of MB and RhB solutions utilizing Co-CdSe@ECNFs under visible light irradiation at different time intervals is shown in Figure 9c,d. As can be seen, with the increase in irradiation time, all the corresponding absorbance peaks of MB and RhB solutions located at 665 nm and 554 nm were observed to gradually diminish. Furthermore, the color of the corresponding dye solutions gradually weakened with time in the presence of Co-CdSe@ECNFs (insets, Figure 9c,d). Besides photocatalytic efficiency, the stability of the photocatalyst is another important aspect for practical application. Therefore, cycling experiments for MB and RhB degradation utilizing Co-CdSe@ECNFs were conducted under visible light irradiation. For cycling experiments, the used sample was centrifuged and dried at room temperature. Based on the results (Figure 10a,b), the photocatalytic performance of Co-CdSe@ECNFs was found to be stable up to the third cycle, but there was a slight decrease in activity during cycling experiments, which could be due to the loss of photocatalyst during the separation process. The reaction kinetics of MB and RhB photodegradation utilizing Co-CdSe@ECNFs and CdSe@ECNFs were calculated with the Langmuir-Hinshelwood equation.

1
(1) Besides photocatalytic efficiency, the stability of the photocatalyst is another important aspect for practical application. Therefore, cycling experiments for MB and RhB degradation utilizing Co-CdSe@ECNFs were conducted under visible light irradiation. For cycling experiments, the used sample was centrifuged and dried at room temperature. Based on the results (Figure 10a,b), the photocatalytic performance of Co-CdSe@ECNFs was found to be stable up to the third cycle, but there was a slight decrease in activity during cycling experiments, which could be due to the loss of photocatalyst during the separation process. The reaction kinetics of MB and RhB photodegradation utilizing Co-CdSe@ECNFs and CdSe@ECNFs were calculated with the Langmuir-Hinshelwood equation.
Here, Co, Ct, and kapp represent the initial concentration, concentration at time t (min), and apparent rate constant (min −1 ), respectively. The kapp is determined by plotting the graph of ln(Co/Ct) vs. reaction time. The photodegradation kinetics of MB and RhB were calculated using Equation (2), and results are presented in Figure 10c,d. The linear relationship of ln(Co/C) vs. reaction time could suggest the pseudo-first-order kinetics of the photodegradation reaction. The apparent rate constants of MB and RhB degradation over Co-CdSe@ECNFs were determined to be 0.035 min −1 and 0.022 min −1 , respectively. Likewise, the apparent rate constants of MB and RhB degradation over CdSe@ECNFs were determined to be 0.028 min −1 and 0.018 min −1 respectively. Thus, the above results signify the role of Co 2+ as a dopant for enhancing the photocatalytic activity of Co-CdSe@ECNFs under visible light irradiation. The possible mechanism scheme for enhanced photocatalytic activity of Co-CdSe@ECNFs is shown in Figure 11. When Co-CdSe@ECNFs photocatalyst was irradiated with visible light, electrons (e -) from the valence band (VB) of Co-CdSe were excited to the conduction band (CB), leaving behind holes (h + ). Some of the excited electrons in CB reacted directly with dissolved oxygen to generate reactive oxygen species (ROS), that is, oxygen peroxide radicals (O2 ᆞ− ), because of the more negative ECB of Co-CdSe than O2/O2 ᆞ− potential (−0.33 eV versus normal hydrogen electrode (NHE)), while other electrons transferred to the ECNFs due to their good electrical conductivity and close attachment with Co-CdSe nanoparticles. Transferred electrons also reacted with oxygen to generate O2 ᆞ− . Additionally, doped Co 2+ could play an important role in capturing and transferring electrons to prevent the recombination of photogenerated charge carriers [46]. Thus, ROS produced during the reaction process are responsible for the photodegradation of MB dye and RhB [47]. As the initial concentration of MB and RhB solutions were very low (C o = 10 mg/L), Equation (1) was reduced to a pseudo-first-order kinetics equation [45] as: Here, C o , C t , and k app represent the initial concentration, concentration at time t (min), and apparent rate constant (min −1 ), respectively. The k app is determined by plotting the graph of ln(C o /C t ) vs. reaction time. The photodegradation kinetics of MB and RhB were calculated using Equation (2), and results are presented in Figure 10c,d. The linear relationship of ln(C o /C) vs. reaction time could suggest the pseudo-first-order kinetics of the photodegradation reaction. The apparent rate constants of MB and RhB degradation over Co-CdSe@ECNFs were determined to be 0.035 min −1 and 0.022 min −1 , respectively. Likewise, the apparent rate constants of MB and RhB degradation over CdSe@ECNFs were determined to be 0.028 min −1 and 0.018 min −1 respectively. Thus, the above results signify the role of Co 2+ as a dopant for enhancing the photocatalytic activity of Co-CdSe@ECNFs under visible light irradiation.
The possible mechanism scheme for enhanced photocatalytic activity of Co-CdSe@ECNFs is shown in Figure 11. When Co-CdSe@ECNFs photocatalyst was irradiated with visible light, electrons (e − ) from the valence band (VB) of Co-CdSe were excited to the conduction band (CB), leaving behind holes (h + ). Some of the excited electrons in CB reacted directly with dissolved oxygen to generate reactive oxygen species (ROS), that is, oxygen peroxide radicals (O 2 •− ), because of the more negative E CB of Co-CdSe than O 2 /O 2 •− potential (−0.33 eV versus normal hydrogen electrode (NHE)), while other electrons transferred to the ECNFs due to their good electrical conductivity and close attachment with Co-CdSe nanoparticles. Transferred electrons also reacted with oxygen to generate O 2 •− . Additionally, doped Co 2+ could play an important role in capturing and transferring electrons to prevent the recombination of photogenerated charge carriers [46]. Thus, ROS produced during the reaction process are responsible for the photodegradation of MB dye and RhB [47]. Conversely, photogenerated holes in the VB of Co-CdSe could not react with water to generate hydroxyl radicals (OH • ) as the E VB was more negative than the OH • /OH − potential (2.38 eV versus an NHE) [48]. As a consequence, holes were involved in the reduction reaction directly.
Catalysts 2020, 10, 348 11 of 15 Conversely, photogenerated holes in the VB of Co-CdSe could not react with water to generate hydroxyl radicals (OH ᆞ ) as the EVB was more negative than the OH ᆞ /OH − potential (2.38 eV versus an NHE) [48]. As a consequence, holes were involved in the reduction reaction directly.

Fabrication of Ternary Composite of Co-CdSe@ECNFs
Ternary composite of Co-CdSe@ECNFs was prepared by electrospinning followed by carbonization. For the fabrication of Co 2+ /Cd 2+/ Se PAN precursor nanofibers, first, 1 mmol of Se powder was dispersed in 12 g of DMF, then 1 mmol of cobalt acetate and 1 mmol of cadmium acetate were added to the above solution with strong magnetic stirring for 1 h. Finally, 1 g of PAN was added to the mixture solution and left for 12 h of continuous magnetic stirring in order to obtain a homogeneous solution. The final solution was loaded into a 5 mL injection syringe provided with a plastic micro-tip, and electrospinning of the precursor solution was carried out using a high voltage power supply at an applied voltage of 18 kV. In this process, the distance between the tip and collector was kept at 12 cm, while the developing electrospun nanofibers were collected on a drum collector which was rotated at a constant speed by a DC motor. All the experimental works were conducted at room temperature and atmospheric pressure. The electrospun nanofibers were vacuum dried at 70 °C for 12 h to remove the residual solvent. For carbonization, vacuum-dried electrospun precursor nanofibers were stabilized at 250 °C for 2 h with a heating rate of 1 °C/min and cooled to room temperature, they were then carbonized in Ar atmosphere at 800 °C for 2 h with a heating rate of 5 °C/min. After cooling to room temperature, ternary composite of Co-CdSe@ECNFs was obtained. For comparison, composite of CdSe@ECNFs was prepared under similar conditions without adding Co 2+ . All the chemicals were used as received without further purification.

Fabrication of Ternary Composite of Co-CdSe@ECNFs
Ternary composite of Co-CdSe@ECNFs was prepared by electrospinning followed by carbonization. For the fabrication of Co 2+ /Cd 2+ /Se PAN precursor nanofibers, first, 1 mmol of Se powder was dispersed in 12 g of DMF, then 1 mmol of cobalt acetate and 1 mmol of cadmium acetate were added to the above solution with strong magnetic stirring for 1 h. Finally, 1 g of PAN was added to the mixture solution and left for 12 h of continuous magnetic stirring in order to obtain a homogeneous solution. The final solution was loaded into a 5 mL injection syringe provided with a plastic micro-tip, and electrospinning of the precursor solution was carried out using a high voltage power supply at an applied voltage of 18 kV. In this process, the distance between the tip and collector was kept at 12 cm, while the developing electrospun nanofibers were collected on a drum collector which was rotated at a constant speed by a DC motor. All the experimental works were conducted at room temperature and atmospheric pressure. The electrospun nanofibers were vacuum dried at 70 • C for 12 h to remove the residual solvent. For carbonization, vacuum-dried electrospun precursor nanofibers were stabilized at 250 • C for 2 h with a heating rate of 1 • C/min and cooled to room temperature, they were then carbonized in Ar atmosphere at 800 • C for 2 h with a heating rate of 5 • C/min. After cooling to room temperature, ternary composite of Co-CdSe@ECNFs was obtained. For comparison, composite of CdSe@ECNFs was prepared under similar conditions without adding Co 2+ .

Characterization
The crystalline phase of samples was investigated by an X-ray diffractometer (XRD, Empyrean, PANAlytical, Eindhoven 5651 GH, Netherlands) with Cu Kα (λ = 1.540 Å) radiation over Bragg angles ranging from 10 • to 70 • . Field-emission scanning electron microscopy (FESEM, GeminiSEM 500, Carl Zeiss Microscopy GmbH, 73447 Oberkochen, Germany) equipped with energy-dispersive X-ray spectroscopy (EDS) was used to study the morphology and to analyze the elemental composition of the samples. Transmission electron microscopy was applied to study the morphology and distribution of nanoparticles on ECNFs. Additionally, high-resolution images (HR-TEM) of the prepared sample were observed using a transmission electron microscope (TEM, JEM-2200FS, JEOL Ltd., Akishima, Tokyo, Japan) equipped with EDS. The surface element composition analysis of Co-CdSe@ECNFs was recorded using X-ray photoelectron spectroscopy (XPS, AXIS-NOVA, Kratos Analytical Ltd., Manchester, M17 1GP, UK). Raman spectroscopy was utilized to determine the degree of disorder and the composition of the samples using a micro-Raman spectrometer (Tokyo instrument, Nanofinder 30, Tokyo, Japan). UV-Vis diffusive reflectance spectra (DSR) of composites were measured using a UV-Vis spectrophotometer (UV-2600 240 EN, SHIMADZU CORPORATION, Kyoto, Japan).

Photocatalytic Activity Investigation
Photocatalytic activities of CdSe@ECNFs and Co-CdSe@ECNFs were investigated by observing the degradation of MB and RhB dye solutions using a solar simulator with an internal xenon lamp (DYX300P, DYE TECH Co., Seoul, Korea) equipped with a UV cut-off filter. In this experiment, 50 mL of dye solution, with an initial concentration of 10 mg L −1 was mixed with 50 mg of photocatalyst in a glass vial and magnetically stirred for 30 min under dark conditions in order to establish an adsorption/desorption equilibrium between dye molecules and photocatalysts. After that, visible light (λ > 420 nm) obtained from a 200 W xenon lamp was irradiated under constant magnetic stirring. In order to investigate the self-degradation of dye solutions under identical conditions, blank tests were performed without utilizing photocatalyst. Aliquots were taken at regular time intervals and the concentration of the dye solution was measured spectrophotometrically by recording the absorbance using a UV-Vis spectrophotometer (HP 8453 UV-Vis spectroscopy system, Hudson, MA, USA).

Conclusions
This research aimed to present a successful effort towards fabricating a ternary composite with inorganic-organic heterostructure composed of in-situ-synthesized Co-CdSe nanoparticles and ECNFs using electrospinning followed by carbonization. All the samples were characterized using FESEM, XRD, TEM, XPS, Raman spectroscopy, and UV-Vis spectroscopy. Thus, the obtained ternary composites (Co-CdSe@ECNFs) showed enhanced photocatalytic activity towards the photodegradation of MB and RhB under visible light due to sufficient electron-hole separation ability, compared to that of CdSe@ECNFs. Similarly, a large length-to-diameter ratio of ECNFs could make the separation process of photocatalyst simpler after use. Finally, the impact of Co doping on the photocatalytic activity of ternary composite has been reported.
Author Contributions: For this research article, the individual contribution of authors was as follows: conceptualization and data analysis, G.P. and K.R.G.; methodology, G.P., O.H.K., Y.W.P., and Y.-S.K.; manuscript preparation, G.P. and K.R.G.; writing-review and editing, G.P. and M.P.; resources and supervision, M.P.; funding acquisition, M.P. All authors have read and agreed to the published version of the manuscript.