Computational Study of Novel Semiconducting Sc2CT2 (T = F, Cl, Br) MXenes for Visible-Light Photocatalytic Water Splitting

Seeking candidate photocatalysts for photocatalytic water splitting, via visible light, is of great interest and importance. In this study, we have comprehensively explored the crystal structures, electronic properties, and optical absorbance of two-dimensional (2D) Sc2CT2 (T = F, Cl, Br) MXenes and their corresponding photocatalytic water splitting, under the visible-light region, by first-principles calculations. Herein, we have proposed that 2D Sc2CT2 MXenes can be fabricated from their layered bulk compounds, alternatively to the traditional chemical etching method. Creatively, we proposed Sc2CT2 (T = F, Br) as new materials; the band edge alignments of Sc2CF2 can be tuned to meet the water redox potentials at pH = 8.0. It is highlighted that Sc2CF2 shows outstanding optical spectra harvested under visible-light wavelength regions, and efficient separation of photo-induced electrons and holes in different zones. These present results provide eloquent evidence and open a new door on the photocatalysis applications of such novel semiconducting MXenes.


Introduction
Hydrogen production, through photocatalytic water splitting via visible-light irradiation, is a promising solution to solve the environmental issues by achieving low-cost, nonpolluting, and environmentally friendly energy [1,2]. A suitable photocatalyst must fulfill at least the following three requirements: moderate band gaps, appropriate band alignments, and efficient separation of photo-generated electron-hole pairs. This is to say, the band gap of the semiconductor photocatalyst must straddle the redox potential of water, as follows: the conduction band minimum (CBM) must be higher than −4.44 eV, which is the redox potential of H + /H 2 ; and the valence band maximum (VBM) must be lower than −5.67 eV, which is the redox potential of H 2 O/O 2 [3][4][5]. Accordingly, 1.23 eV is the smallest band gap for a semiconductor photocatalyst. To exploit solar radiation more efficiently, a value of around 1.8 eV is an ideal gap for an efficient photocatalyst [2,6,7]. Moreover, the efficiency of a photocatalyst must always be hampered by the recombination of photo-induced electron-hole pairs. Therefore, the efficient carrier separation is another vital point in semiconductor photocatalysts. However, finding an efficient semiconductor photocatalyst for hydrogen generation, to meet all the above requirements, is still an ongoing challenge [5].
Recently, two-dimensional (2D) transition metal carbides/nitrides (MXene) were produced from their corresponding MAX phases, where M stands for early transition metal, A stands for IIIA or IVA element, and X represents C or N [8][9][10][11][12][13][14][15][16]. MXenes have been extensively explored for miscellaneous applications as photocatalysts [17][18][19], electromagnetic interference shielding [20], battery anodes [21,22], heavy-metal removal [23], etc. Especially, for the photocatalytic community, monolayer Zr 2 CO 2 and Hf 2 CO 2 MXenes have been evaluated as semiconductor photocatalysts. They not only exhibit suitable band gaps and band alignments, but can also separate photo-generated electrons and holes effectively [17][18][19]. Except for Zr 2 CO 2 and Hf 2 CO 2 , the semiconducting feature was characterized in some other Sc-based MXenes, such as Sc 2 CO 2 and Sc 2 C(OH) 2 , which possess the band gaps of 2.96 eV and 0.77 eV, respectively [24,25]. Experimentally, a layered Sc 2 CCl 2 bulk crystal, with a unit cell that is isostructural to a 2D MXene, was successfully synthesized, which implied the feasibility for the fabrication of monolayer Sc 2 CCl 2 [26]. Theoretically, the calculated optical bandgap of one-layer (1 L), 2 L and 3 L Sc 2 CCl 2 is about 1.5 eV by the GW + RPA method [27]. Accordingly, the monolayer Sc 2 CCl 2 is a promising optoelectronic material, due to the excellent light absorbance [27]. In addition, the analogue bulk crystal Y 2 CF 2 has been directly synthesized through a high-temperature solid-state reaction a while ago [28,29]. The crystal has the ability to photo-reduce protons into H 2 in the range of visible light [28]. Inspired by these studies, and considering the analogous of F, Cl, and Br, we wonder if Sc 2 CT 2 MXenes (T = F, Cl, Br) are endowed with outstanding features as efficient semiconductor photocatalysts for water splitting.
Thanks to the progress of the density functional theory, the computational method is now a very important approach for designing new functional material. In the present work, we have comprehensively explored the exfoliate energy, geometrical structure, kinetic and thermal stabilities, as well as electronic properties and optical absorbance of 2D Sc 2 CT 2 (T = F, Cl, Br) MXenes, using first-principles calculations. Especially, we have extensively explored the possibility of Sc 2 CT 2 (T = F, Cl, Br) MXenes to be used for visible-light photocatalytic water splitting. Our study can make contributions to the discovery and applications of Sc-based MXenes, as semiconductor photocatalysts for water-splitting hydrogen production.

Methods
Our first-principles calculations were performed using the projector augmentedwave (PAW) [30] of generalized gradient approximation (GGA) with Perdew-Burke-Ernzerhof (PBE) [31] formalism, implemented in the Vienna ab initio simulation package (VASP) [32,33]. The energy cutoff of the plane-wave expansion was 550 eV. The thickness of the vacuum space was 25 Å in the z direction. The reciprocal space was represented by a Monkhorst-Pack scheme with 11 × 11 × 1 k-point grid meshes. The convergence criteria of energy for both electrons and ions were, respectively, 1 × 10 −5 eV and 1 × 10 −6 eV. Phonon dispersions were retrieved by the density functional perturbation theory (DFPT) as embedded in the PHONOPY code to study the kinetic stability [34,35], for which a 4 × 4 × 1 supercell with 4 × 4 × 1 k-point grid meshes was employed. The DFT-D3 van der Waals (vdW)-corrected methods [36] were performed for the improved descriptions of the layered bulk crystals. The calculation results were dealt by the ALKEMIE code [37]. To obtain accurate dielectric functions, we employed the time-dependent Hartree-Fock calculations (TDHF) [38] by the Heyd-Scuseria-Ernzerhof (HSE06) [39] calculations, which have taken the excitonic effects into account.

Results and Discussion
First, the bulk and monolayer structures of Sc 2 CT 2 (T = F, Cl, Br) are displayed in Figure 1. The bulk phase is crystallized in the trigonal space group of P3m1, in which the upper and lower sides of the Sc 2 C plane are halogenated by two T atomic layers. Moreover, the center C atoms are coordinated by six Sc atoms, leading to an octahedron of Sc 6 C. Table 1 lists the calculated lattice parameters a (Å) and Sc-C bond lengths L (Å) of the Sc 6 C octahedron of the monolayer Sc 2 CT 2 . The lattice parameters a (Å) and c (Å) of the bulk Sc 2 CT 2 are listed for comparison as well. According to our calculations, the lattice constant, via the structural optimization for bulk Sc 2 CCl 2 , is 3.445 Å, which is in line with the experimental result [26]. As the surface groups change from F to Br, the lattice parameters increase slightly, which is attributed to the raising of the halogen element atomic radius. In the Sc 6 C octahedron of the monolayer Sc 2 CT 2 , the changes in the Sc-C bond lengths show the same trend as the surface groups from F to Br. It is worth noting that the calculated lattice parameters a of the monolayer Sc 2 CT 2 are almost identical with that of their bulk phases, indicating that the interlayer interaction between the atomic layers are very weak. Thus, the monolayer Sc 2 CT 2 is likely to be isolated from the corresponding bulk phase. Sc2CT2 are listed for comparison as well. According to our calculations, the lattice constant, via the structural optimization for bulk Sc2CCl2, is 3.445 Å, which is in line with the experimental result [26]. As the surface groups change from F to Br, the lattice parameters increase slightly, which is attributed to the raising of the halogen element atomic radius. In the Sc6C octahedron of the monolayer Sc2CT2, the changes in the Sc-C bond lengths show the same trend as the surface groups from F to Br. It is worth noting that the calculated lattice parameters a of the monolayer Sc2CT2 are almost identical with that of their bulk phases, indicating that the interlayer interaction between the atomic layers are very weak. Thus, the monolayer Sc2CT2 is likely to be isolated from the corresponding bulk phase.  Herein, the 3D bulk crystals are composed of stacked MXene sheets, as displayed in Figure 1. Distinct from the traditional chemical etching method to fabricate MXene, which is environmentally unfriendly, owing to the using of hydrofluoric acid (HF), we introduce an alternative isolation approach, which has been successfully used for graphene manufacturing. Figure 2 displays the calculated exfoliation energy of Sc2CT2, and the exfoliation energy of graphite is also shown as a benchmark. As is observed, the evaluated exfoliation energy of graphite is ~0.32 J/m 2 , according to our calculation, which is consistent with the experimental measurement and previous theoretical study [40,41]. Amazedly, the calculated exfoliation energies for all the explored Sc2CT2 are much lower than that of graphite, suggesting that the monolayer Sc2CT2 is very likely to be obtained from its bulk phases, by similar experimental methods as graphene. Especially, the exfoliation energy of Sc2CF2 is only ~0.23 J/m 2 . Such value is nearly two-thirds of that for graphite, indicating the ranking possibility for experimental fabrication.  Herein, the 3D bulk crystals are composed of stacked MXene sheets, as displayed in Figure 1. Distinct from the traditional chemical etching method to fabricate MXene, which is environmentally unfriendly, owing to the using of hydrofluoric acid (HF), we introduce an alternative isolation approach, which has been successfully used for graphene manufacturing. Figure 2 displays the calculated exfoliation energy of Sc 2 CT 2 , and the exfoliation energy of graphite is also shown as a benchmark. As is observed, the evaluated exfoliation energy of graphite is~0.32 J/m 2 , according to our calculation, which is consistent with the experimental measurement and previous theoretical study [40,41]. Amazedly, the calculated exfoliation energies for all the explored Sc 2 CT 2 are much lower than that of graphite, suggesting that the monolayer Sc 2 CT 2 is very likely to be obtained from its bulk phases, by similar experimental methods as graphene. Especially, the exfoliation energy of Sc 2 CF 2 is only~0.23 J/m 2 . Such value is nearly two-thirds of that for graphite, indicating the ranking possibility for experimental fabrication.
The stability acts a pivotal part in the practical application and experimental fabrication of 2D Sc 2 CT 2 . Therefore, the phonon dispersion spectra calculations were employed, to assess the kinetic stabilities of 2D Sc 2 CT 2 . Moreover, ab initio molecular dynamics (AIMD) calculations were adopted, to evaluate the thermal stabilities. As the phonon curves illustrated in the upper panel of Figure 3, there is not any appreciable imaginary acoustic dispersion branch of the phonon curve for all the Sc 2 CT 2 , confirming the kinetic stabilities of the three monolayer MXenes. More importantly, the highest phonon spectra frequencies of all the investigated Sc 2 CT 2 are up to 20 THz. This value is comparable with that of the other monolayer material, implying the rough junction among the Sc, C, and T atoms [19]. The total energy changes and structure snapshots at 300 K, sustaining 9 ps of Sc 2 CT 2 , are displayed in the lower panel of Figure 3. As is shown, the total energies are swinging very slightly and the atoms are well maintained around their equilibrium positions under the temperature field, indicating the thermal stabilities of the monolayer Sc 2 CT 2 . Hence, the kinetic stabilities and thermal stabilities of the Sc 2 CT 2 monolayer have been approved. The stability acts a pivotal part in the practical application and experimental fabrication of 2D Sc2CT2. Therefore, the phonon dispersion spectra calculations were employed, to assess the kinetic stabilities of 2D Sc2CT2. Moreover, ab initio molecular dynamics (AIMD) calculations were adopted, to evaluate the thermal stabilities. As the phonon curves illustrated in the upper panel of Figure 3, there is not any appreciable imaginary acoustic dispersion branch of the phonon curve for all the Sc2CT2, confirming the kinetic stabilities of the three monolayer MXenes. More importantly, the highest phonon spectra frequencies of all the investigated Sc2CT2 are up to 20 THz. This value is comparable with that of the other monolayer material, implying the rough junction among the Sc, C, and T atoms [19]. The total energy changes and structure snapshots at 300 K, sustaining 9 ps of Sc2CT2, are displayed in the lower panel of Figure 3. As is shown, the total energies are swinging very slightly and the atoms are well maintained around their equilibrium positions under the temperature field, indicating the thermal stabilities of the monolayer Sc2CT2. Hence, the kinetic stabilities and thermal stabilities of the Sc2CT2 monolayer have been approved.   The stability acts a pivotal part in the practical application and experimental fabrication of 2D Sc2CT2. Therefore, the phonon dispersion spectra calculations were employed, to assess the kinetic stabilities of 2D Sc2CT2. Moreover, ab initio molecular dynamics (AIMD) calculations were adopted, to evaluate the thermal stabilities. As the phonon curves illustrated in the upper panel of Figure 3, there is not any appreciable imaginary acoustic dispersion branch of the phonon curve for all the Sc2CT2, confirming the kinetic stabilities of the three monolayer MXenes. More importantly, the highest phonon spectra frequencies of all the investigated Sc2CT2 are up to 20 THz. This value is comparable with that of the other monolayer material, implying the rough junction among the Sc, C, and T atoms [19]. The total energy changes and structure snapshots at 300 K, sustaining 9 ps of Sc2CT2, are displayed in the lower panel of Figure 3. As is shown, the total energies are swinging very slightly and the atoms are well maintained around their equilibrium positions under the temperature field, indicating the thermal stabilities of the monolayer Sc2CT2. Hence, the kinetic stabilities and thermal stabilities of the Sc2CT2 monolayer have been approved.  To understand the electronic properties of monolayer Sc 2 CT 2 , the total and partial density of states (DOS) are represented in Figure 4. Note that the DOS of Sc 2 CF 2 , Sc 2 CCl 2 , and Sc 2 CBr 2 exhibit very similar features, which is in relation to their alike atomic configurations. For the explored Sc 2 CF 2 and Sc 2 CCl 2 , the CBM is mainly contributed by Sc 3d states, while the VBM is entirely dominated by C 2p states and Sc 3d states. In addition, the C 2p orbits and Sc 3d orbits are forcefully hybridized [42]. The CBM of Sc 2 CBr 2 is contributed by Sc 3d states as well, but the VBM of it is not only dominated by C 2p states and Sc 3d states, but also contributed by Br 4p states. Moreover, the calculated band gaps for Sc 2 CF 2 , Sc 2 CCl 2 , and Sc 2 CBr 2 are 1.85 eV, 1.70 eV, and 1.54 eV, respectively, which are endowed with high harvest under the visible-light region. Note that the band gaps of all three 2D Sc 2 CT 2 are larger than 1.23 eV, which meet the minimum value required for an efficient photocatalyst. Hence, it can be concluded that all the Sc 2 CT 2 MXenes are promising candidates as semiconductor photocatalysts, in the aspect of bandgaps.
states, while the VBM is entirely dominated by C 2p states and Sc 3d states. In addition, the C 2p orbits and Sc 3d orbits are forcefully hybridized [42]. The CBM of Sc2CBr2 is contributed by Sc 3d states as well, but the VBM of it is not only dominated by C 2p states and Sc 3d states, but also contributed by Br 4p states. Moreover, the calculated band gaps for Sc2CF2, Sc2CCl2, and Sc2CBr2 are 1.85 eV, 1.70 eV, and 1.54 eV, respectively, which are endowed with high harvest under the visible-light region. Note that the band gaps of all three 2D Sc2CT2 are larger than 1.23 eV, which meet the minimum value required for an efficient photocatalyst. Hence, it can be concluded that all the Sc2CT2 MXenes are promising candidates as semiconductor photocatalysts, in the aspect of bandgaps. Besides the bandgap size, band edge alignments are another predominant factor to facilitate the water reaction. We have therefore calculated the band edge alignments of Sc2CT2 in Figure 5, to assess the performance of these newly designed photocatalysts. According to the band alignments in Figure 5, 2D Sc2CCl2 and Sc2CBr2 exhibit very similar band edge alignment characters. Interestingly, the VBM of Sc2CCl2 and Sc2CBr2 are located at a more positive potential than the water redox potential of H2O/O2 (1.23 eV vs. normal hydrogen electrode, NHE), implying the remarkable oxidation capabilities of the photogenerated holes. This advantage can be applied in capturing the electrons from organic pollutants, such as methylene blue [19]. However, it is a pity that the CBMs of Sc2CT2 are also located at a more positive potential than the redox potential of H + /H2 (0 V vs. NHE), indicating that they are not appropriate for photocatalytic water splitting. While for Sc2CF2, the CBM is much more negative than the redox potential of H + /H2 (0 V vs. NHE), but the VBM position is not more positive than the redox potential of O2/H2O (1.23 eV vs. NHE), suggesting the unapplicable band alignments for water splitting. From the above analysis, one can observe that the band positions of 2D Sc2CF2, Sc2CCl2 and Sc2CBr2 are not suitable as semiconductor photocatalysts under ambition conditions. Besides the bandgap size, band edge alignments are another predominant factor to facilitate the water reaction. We have therefore calculated the band edge alignments of Sc 2 CT 2 in Figure 5, to assess the performance of these newly designed photocatalysts. According to the band alignments in Figure 5, 2D Sc 2 CCl 2 and Sc 2 CBr 2 exhibit very similar band edge alignment characters. Interestingly, the VBM of Sc 2 CCl 2 and Sc 2 CBr 2 are located at a more positive potential than the water redox potential of H 2 O/O 2 (1.23 eV vs. normal hydrogen electrode, NHE), implying the remarkable oxidation capabilities of the photogenerated holes. This advantage can be applied in capturing the electrons from organic pollutants, such as methylene blue [19]. However, it is a pity that the CBMs of Sc 2 CT 2 are also located at a more positive potential than the redox potential of H + /H 2 (0 V vs. NHE), indicating that they are not appropriate for photocatalytic water splitting. While for Sc 2 CF 2 , the CBM is much more negative than the redox potential of H + /H 2 (0 V vs. NHE), but the VBM position is not more positive than the redox potential of O 2 /H 2 O (1.23 eV vs. NHE), suggesting the unapplicable band alignments for water splitting. From the above analysis, one can observe that the band positions of 2D Sc 2 CF 2 , Sc 2 CCl 2 and Sc 2 CBr 2 are not suitable as semiconductor photocatalysts under ambition conditions. From Figure 5, the band alignments of Sc2CF2 are not appropriate under ambient conditions. However, in the practical application of a photocatalysis, the water redox potential is related to the value of pH in the solutions. Hence, the water oxidation potential of O2/H2O can be expressed by the following equation [43]:  Figure 5, the band alignments of Sc 2 CF 2 are not appropriate under ambient conditions. However, in the practical application of a photocatalysis, the water redox potential is related to the value of pH in the solutions. Hence, the water oxidation potential of O 2 /H 2 O can be expressed by the following equation [43]: According to Equation (1), one can shift the oxidation level of water upward in Figure 5. Thus, the band edge alignments of Sc 2 CF 2 can be tuned to straddle the redox potential of water. As illustrated in Figure 6, in ambient conditions, Sc 2 CF 2 is not an appropriate photocatalyst, due to its unsuitable band edge alignments. While in a pH = 8.0 solution, the oxidation level and the reduction potential of water will shift upwards by 0.472 V. We have plotted the band alignments of Sc 2 CF 2 in Figure 6, from which one can observe that the VBM locates more positively than the hydrogen reduction level (0 V vs. NHE), and the CBM locates more negatively than the oxygen oxidation level (1.23 eV vs. NHE). The results show that Sc 2 CF 2 has a favorable band position for water splitting in a pH = 8.0 solution. Moreover, the energy difference between VBM and the oxygen reduction potential (oxidizing power) of Sc 2 CF 2 is 0.25 eV, and the energy difference between CBM and the hydrogen reduction potential (reducing power) is 0.38 eV. Furthermore, we can moderate the water-oxidizing power and reducing power of Sc 2 CF 2 by changing the pH to 9.0. Notably, the oxidizing power increases to 0.31 eV, while the reducing power decreases to 0.32 eV. Such values suggest that Sc 2 CF 2 has excellent band edge positions as photocatalysts, which is very helpful for protecting the chemical equilibriums during the water-splitting reaction process. From Figure 5, the band alignments of Sc2CF2 are not appropriate under ambient conditions. However, in the practical application of a photocatalysis, the water redox potential is related to the value of pH in the solutions. Hence, the water oxidation potential of O2/H2O can be expressed by the following equation [43]: According to Equation (1), one can shift the oxidation level of water upward in Figure  5. Thus, the band edge alignments of Sc2CF2 can be tuned to straddle the redox potential of water. As illustrated in Figure 6, in ambient conditions, Sc2CF2 is not an appropriate photocatalyst, due to its unsuitable band edge alignments. While in a pH = 8.0 solution, the oxidation level and the reduction potential of water will shift upwards by 0.472 V. We have plotted the band alignments of Sc2CF2 in Figure 6, from which one can observe that the VBM locates more positively than the hydrogen reduction level (0 V vs. NHE), and the CBM locates more negatively than the oxygen oxidation level (1.23 eV vs. NHE). The results show that Sc2CF2 has a favorable band position for water splitting in a pH = 8.0 solution. Moreover, the energy difference between VBM and the oxygen reduction potential (oxidizing power) of Sc2CF2 is 0.25 eV, and the energy difference between CBM and the hydrogen reduction potential (reducing power) is 0.38 eV. Furthermore, we can moderate the water-oxidizing power and reducing power of Sc2CF2 by changing the pH to 9.0. Notably, the oxidizing power increases to 0.31 eV, while the reducing power decreases to 0.32 eV. Such values suggest that Sc2CF2 has excellent band edge positions as photocatalysts, which is very helpful for protecting the chemical equilibriums during the watersplitting reaction process.  Having confirmed the band gap and band edge alignments of Sc 2 CF 2 , we now turn to its optical spectra in the visible-light wavelength range, which is another vital criteria for photocatalysts to drive the water-splitting reaction efficiently. Figure 7 displays the optical absorbance of Sc 2 CF 2 , obtained from TDHF-HSE06 and DFT-HSE06, and the light spectrum of silicon is plotted as a benchmark [44]. As is observed, the calculated optical absorbance of 2D Sc 2 CF 2 are absolutely higher than that of silicon, in most visible-light regions. Moreover, the optical absorption, obtained by the TDHF-HSE06 method, is significantly larger than that evaluated by the standard DFT-HSE06 approach, which implies a strong excitonic effect in Sc 2 CF 2 , in the visible-light region. For the absorption coefficients that were evaluated by the TDHF-HSE06 method, 2D Sc 2 CF 2 exhibits broad optical absorptions, with three optical spectra peaks at around~400 nm,~450 nm, and~550 nm. It is worth noting that the optical coefficients of Sc 2 CF 2 can reach up to~2 × 10 5 cm −1 at around~550 nm, suggesting an extraordinary light harvesting ability. The outstanding optical performances imply that the Sc 2 CF 2 monolayer is a very hopeful candidate as a semiconductor photocatalyst for hydrogen generation. a strong excitonic effect in Sc2CF2, in the visible-light region. For the absorption coefficients that were evaluated by the TDHF-HSE06 method, 2D Sc2CF2 exhibits broad optical absorptions, with three optical spectra peaks at around ~400 nm, ~450 nm, and ~550 nm. It is worth noting that the optical coefficients of Sc2CF2 can reach up to ~2 × 10 5 cm −1 at around ~550 nm, suggesting an extraordinary light harvesting ability. The outstanding optical performances imply that the Sc2CF2 monolayer is a very hopeful candidate as a semiconductor photocatalyst for hydrogen generation. The efficient separation of photo-induced electrons and holes can guarantee high efficiency of a semiconductor photocatalyst. Figure 8a shows the electron localization functions (ELFs) of 2D Sc2CF2, to investigate the spatial charge distributions. As presented in Figure 8a, the electrons are transferred from Sc atoms to C atoms and F atoms, and completely gathered around C atoms and F atoms, leading to highly localized surroundings. Accordingly, the positively charged region around the Sc atoms will attract the photogenerated electrons, while the negatively charged region around the C and F atoms will trap the photo-activated holes. Hence, the photo-induced electron-hole pairs tend to aggregated in different areas, resulting in efficient carrier separation in the Sc2CF2 monolayer. As is known, most photo-generated electrons are gathered at the CBM, and photogenerated holes are gathered at the VBM [4,46]. We have then computed the band decomposed charge density of the Sc2CF2 material in Figure 8. From the band decomposed charge density, we can observe that the CBMs are entirely contributed by the d electrons from the Sc atoms, while the VBMs are completely dominated by the Sc atoms and p electrons from the C atoms, which is in line with the partial DOS that is displayed in Figure  4a. As is observed, the CBMs are mainly distributed at the Sc-F zones, and the VBM are located at the C zones, thus the photo-induced electrons and holes will transfer to the Sc-F zones and C zones, respectively. Therefore, the photo-excited electron-hole pairs can be separated efficiently at different zones in the monolayer Sc2CF2, which is a benefit for the photocatalysis water-splitting reaction on the monolayer Sc2CF2 photocatalyst. The efficient separation of photo-induced electrons and holes can guarantee high efficiency of a semiconductor photocatalyst. Figure 8a shows the electron localization functions (ELFs) of 2D Sc 2 CF 2 , to investigate the spatial charge distributions. As presented in Figure 8a, the electrons are transferred from Sc atoms to C atoms and F atoms, and completely gathered around C atoms and F atoms, leading to highly localized surroundings. Accordingly, the positively charged region around the Sc atoms will attract the photogenerated electrons, while the negatively charged region around the C and F atoms will trap the photo-activated holes. Hence, the photo-induced electron-hole pairs tend to aggregated in different areas, resulting in efficient carrier separation in the Sc 2 CF 2 monolayer. As is known, most photo-generated electrons are gathered at the CBM, and photo-generated holes are gathered at the VBM [4,46]. We have then computed the band decomposed charge density of the Sc 2 CF 2 material in Figure 8. From the band decomposed charge density, we can observe that the CBMs are entirely contributed by the d electrons from the Sc atoms, while the VBMs are completely dominated by the Sc atoms and p electrons from the C atoms, which is in line with the partial DOS that is displayed in Figure 4a. As is observed, the CBMs are mainly distributed at the Sc-F zones, and the VBM are located at the C zones, thus the photo-induced electrons and holes will transfer to the Sc-F zones and C zones, respectively. Therefore, the photo-excited electron-hole pairs can be separated efficiently at different zones in the monolayer Sc 2 CF 2 , which is a benefit for the photocatalysis water-splitting reaction on the monolayer Sc 2 CF 2 photocatalyst.

Conclusions
In conclusion, we have comprehensively explored the photocatalytic water splitting of Sc2CT2 (T = F, Cl, Br) MXenes, as semiconductor photocatalysts for hydrogen generation, based on first-principles calculations. Firstly, the exfoliation energy of bulk-layered Sc2CT2 has been calculated, which is much smaller than that of graphite, implying that the monolayer Sc2CT2 can be isolated by mechanical cleavage from its bulk phases. Additionally, as demonstrated by phonon calculations and ab initio molecular dynamicssimulations, the Sc2CT2 monolayer shows kinetic and thermal stabilities. Moreover, the calculated band gaps for Sc2CF2, Sc2CCl2, and Sc2CBr2 are 1.85 eV, 1.70 eV, and 1.54 eV, respectively. However, in ambient conditions, Sc2CT2 is not a suitable photocatalyst, due to its inappropriate band edge position. It is highlighted that the band edge alignments of

Conclusions
In conclusion, we have comprehensively explored the photocatalytic water splitting of Sc 2 CT 2 (T = F, Cl, Br) MXenes, as semiconductor photocatalysts for hydrogen generation, based on first-principles calculations. Firstly, the exfoliation energy of bulk-layered Sc 2 CT 2 has been calculated, which is much smaller than that of graphite, implying that the monolayer Sc 2 CT 2 can be isolated by mechanical cleavage from its bulk phases. Additionally, as demonstrated by phonon calculations and ab initio molecular dynamicssimulations, the Sc 2 CT 2 monolayer shows kinetic and thermal stabilities. Moreover, the calculated band gaps for Sc 2 CF 2 , Sc 2 CCl 2 , and Sc 2 CBr 2 are 1.85 eV, 1.70 eV, and 1.54 eV, respectively. However, in ambient conditions, Sc 2 CT 2 is not a suitable photocatalyst, due to its inappropriate band edge position. It is highlighted that the band edge alignments of Sc 2 CF 2 can be tuned to straddle the redox potential of water, by shifting the oxidation level of water upwards, which can be realized by introducing a pH = 8.0 solution. Furthermore, by changing the pH to 9.0, the oxidizing power and reducing power of Sc 2 CF 2 can be moderated to a harmonious level, which is very helpful to keep the chemical balance during the redox reaction. Meanwhile, 2D Sc 2 CF 2 exhibits a high optical absorption, up to 2 × 10 5 cm −1 , in visible-light wavelengths. Notably, the photo-excited electron-hole pairs of Sc 2 CF 2 will separate efficiently. Our exciting results pave the way for designing more MXenes as semiconductor photocatalysts for hydrogen generation.