The structure information of CN and KCN was identified via the XRD, as shown in Fig. 1a, all the diffraction signals of CN and KCN are well matched with the standard pattern of JCPDS 87-1526 (Wang et al., 2020), and peaks located at 12.9° and 27.8° are ascribed to the (100) and (002) plane, respectively. Notably, the characteristic peak of the (002) plane is slightly shifted to lower angle, indicating the interlayer distance of KCN is enlarged, demonstrating that the small sized K atoms enter into the CN structure (Fig. 1b). Furthermore, the weakened (002) peak intensity can be corresponded to the incomplete polymerization induced by the K incorporation during the condensation process. In addition, the chemical structure information of CN and KCN were analyzed by FT-IR, as displayed in Fig. 1c, the characteristic signals at 1200–1650 and 815 cm− 1 are related to the aromatic heterocyclic rings stretching and the heterocyclic ring condensation of triazine unit in g-C3N4 (Li et al., 2007; Zhou et al., 2016). And the apparent peaks of –OH and uncondensed ammonium groups (NH) are observed in 3000–4000 cm− 1 (Bai et al., 2013). Impressively, there is no K-related vibration found in the FT-IR spectra, indicating the introduction of K atoms in CN will not affect the internal chemical deposition.
The XPS spectrum of CN and KCN are further fitted to understand the chemical valence states and element composition. As depicted in Fig. 1d, a pair of apparent K 2p peaks can be fitted in K 2p XPS single, whereas there is no K 2p single in CN sample, indicating the successful introduction of K. Besides, the C 1s fine spectra of CN and KCN (Fig. 1e) can be divided into two obvious peaks, the peak located in 284.5 eV and 284.5 eV are ascribed to the sp2 hybridization of C–C and sp2 hybridization of the carbon (N–C = N) (Li et al., 2014). And in the Fig. 1f, three peaks located at 400.8, 399.0, 398.5 eV in N 1s spectrum can be attributed to N–H of the uncondensed amino groups, tertiary nitrogen in N–(C)3 group, C–N = C group (Gu et al., 2015; Lin and Wang, 2013). Note that the intensity ratio of sp2 N (C–N = C) /sp3 N (N–(C)3) in KCN is 3.95, which is much lower than that in CN (5.79), implying the introduction of K atoms in KCN will cause more structural distortion and defects, as sp2 N becomes sp3 N when the C–N plane is distorted (Wang et al., 2020). As presented by SEM and energy dispersive spectroscopy (EDS) images, the KCN demonstrates the typical morphology of g-C3N4 composed of highly condensed sheets (Fig. 2a). And the EDS mapping demonstrates that the C, N, K elements are uniformly distributed on the surface of KCN (Fig. 2b-d), further confirming the K atoms are successfully inserted into the g-C3N4.
The optical properties of CN and KCN have been investigated by DRS, PL and photo-generate current measurements. As shown in Fig. 3a, CN sample presents a visible light absorption and the edge is located at 478 nm, whereas the KCN shows an apparent shift to larger absorption wavelength at 492 nm, suggesting the electronic structure and band gap are significantly modified in KCN. Further, the energy band gap of CN and KCN are calculated via the Tauc/David–Mott model to be 2.8 eV and 2.7 eV, respectively (Ding et al., 2018), demonstrating that the photocatalytic performance of KCN can be greatly improved via increasing the visible light absorption. Besides, the separation rate of photo-generated electrons/holes in CN and KCN are studied by PL measurement, as depicted in Fig. 3b, the peak at 450 nm can be related to the direct recombination of holes and electrons. And the CN sample displays the lower intensity when comparing with the KCN, indicating the K doping can efficiently depress the recombination of holes and electrons. In addition, the charge separation efficiency can be further confirmed via the photoelectrochemical measurements. As depicted in the photo-generate current response single (conduct at the open circuit potential), it can be found that the photocurrent density of KCN is much higher than that of pure CN, almost two times improved (Fig. 3c). And the EIS plots of CN and KCN are recorded in Fig. 3d, it’s obvious to see that the arc radius of KCN is smaller than that of CN, these results are consistent with photocurrent response and PL results, all implying the K doping in KCN can enhance the visible light absorption range and accelerate the photo-generated carriers transfer, thus improving the photocatalytic activity.
To verify the photocatalytic activity of KCN and CN, the degrading methylene blue dye (MB) efficiency under the visible light were compared. To achieve adsorption-desorption equilibration, the configurations with catalysts and pollutants were stirred for 30 mins in the dark to achieve adsorption-desorption equilibration. As shown in Fig. 4a, the utilization of CN brought 61% removal in 60 mins. In a sharp contrast, the photodegradation of MB was greatly improved in KCN, which achieved a superior removal efficiency of 99% after 60 mins. Furthermore, the photodegradation results were fitted with the fist-order kinetic in Fig. 4b, and rate constant of MB degradation in KCN was about 3.6 times that of CN. To further investigated the positive effect of K incorporation in CN, the KCN with different K content were also conducted the photocatalytic activity. As displayed in Fig. S1, the KCN with 0.1 g potassium sorbate precursor also shows a little enhancement in degradation, whereas the excessive K doping leads to the degradation of catalytic performance in KCN-0.5, which is ascribed to the excessive doping will cause the lattice collapse and affect their performance. After the degradation, the used catalyst was collected and washed, and then reused to check the cycling stability of KCN. In Fig. 4c, the MB removal by KCN could still be maintained above 95% after 5 cycles, indicating an excellent stability of KCN photocatalyst. In addition, to reveal photocatalytic mechanism and reactive species in the degradation system, the ESR spectrums in different configurations were conducted. In ESR spectrum of Fig. 4d, the O2•− intensity in KCN was much stronger than that of CN, means that there were more O2•− generated during the light irradiation, which can be related to the improved conductivity and enhanced photo-generated carriers separation rate. Therefore, more electrons will react with the dissolved O2 to form more O2•− in KCN system (Cao et al., 2019b), thus accelerating the degradation of MB.