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Tuning orbital orientation endows molybdenum disulfide with exceptional alkaline hydrogen evolution capability


Molybdenum disulfide is naturally inert for alkaline hydrogen evolution catalysis, due to its unfavorable water adsorption and dissociation feature originated from the unsuitable orbital orientation. Herein, we successfully endow molybdenum disulfide with exceptional alkaline hydrogen evolution capability by carbon-induced orbital modulation. The prepared carbon doped molybdenum disulfide displays an unprecedented overpotential of 45 mV at 10 mA cm−2, which is substantially lower than 228 mV of the molybdenum disulfide and also represents the best alkaline hydrogen evolution catalytic activity among the ever-reported molybdenum disulfide catalysts. Fine structural analysis indicates the electronic and coordination structures of molybdenum disulfide have been significantly changed with carbon incorporation. Moreover, theoretical calculation further reveals carbon doping could create empty 2p orbitals perpendicular to the basal plane, enabling energetically favorable water adsorption and dissociation. The concept of orbital modulation could offer a unique approach for the rational design of hydrogen evolution catalysts and beyond.


Sustainable hydrogen production in an economical way is the key to building new hydrogen-based energy system1. Water electrolysis driven by renewable energy sources such as solar, wind, or geothermal energy has been regarded as the most promising way for sustainable hydrogen production2,3. Despite the fact that water electrolysis is first discovered in acidic condition, alkaline electrolysis is more preferred in industrial plants, due to the robustness of electrode materials, long lifetime, and cheap electrolyzer construction4. Electrocatalysts, as the heart of the electrolyzers, significantly affect the cell efficiency5. Unfortunately, precious platinum-based materials till now are still the state-of-the-art hydrogen evolution reaction (HER) catalysts in both acidic and alkaline conditions6,7. In this regard, developing non-noble metal-based HER catalysts to replace Pt has been one of the focal points over the past decades8,9,10,11,12,13,14.

Molybdenum disulfide (MoS2), a typical cost-effective layered transition metal dichalcogenide15,16,17,18, has been proved both theoretically and experimentally to be highly active for HER catalysis in acidic condition16,17,18,19,20,21,22,23,24,25,26. The edged Mo and S atoms with a free energy of H adsorption close to zero are commonly believed to be the catalytic sites19,27,28,29,30. Unfortunately, MoS2 is found to be inactive in alkaline condition7,31,32, while the alkaline catalysis is more practically viable. The inert alkaline electrolysis is mainly attributed to the sluggish water adsorption and dissociation dynamics, which is, in essence, determined by the intrinsic structural feature of MoS219,33,34,35. As the dominated orbital compositions of the conduction band in MoS2, both the Mo 4dz2 orbitals in the central sublayer and the S 3px,y orbitals in the outermost sublayers possess unfavorable charge interaction with water molecule due to the steric effect (dz2) and unsuitable orbital orientation (3px,y) in the basal plane, which essentially hinder the water adsorption and dissociation on MoS2 (Fig. 1). Although improving the conductivity of MoS231,36,37 or surface modification with water adsorption components19,33,34 has shown enhanced alkaline electrolysis, the overall performance of MoS2 is still far from being satisfactory for practical alkaline electrolysis and studies on this issue are also very limited. Moreover, the understanding of the alkaline catalytic essences especially at atomic levels is also absent. Therefore, rationally tailoring the catalytic sites to endow MoS2 with efficient alkaline HER catalytic activity is highly desirable but extremely challenging as well.

Fig. 1

The orbital analysis of the MoS2. The top-view (upper) and side-view (lower) orbital compositions of the conduction band in MoS2

To essentially manipulate the intrinsic properties of MoS2 for alkaline HER catalysis, tuning the orbital orientation of the MoS2 layer to promote water adsorption and dissociation dynamics is the key. Considering carbon with smaller atomic radius and less electrons owns more empty and lower-energy 2p valence orbitals than sulfur, partially substituting S with carbon in MoS2 could generate sp2 hybrid sites in the outermost sublayers of MoS2, which consequently vacate one p orbital perpendicular to the basal plane for water adsorption and activation. Herein, we successfully endow MoS2 nanosheets with exceptional alkaline HER activities by carbon-induced surface orbital orientation modulation. Carbon is in-situ incorporated into MoS2 through a unique incomplete sulfurization of Mo2C. The prepared carbon doped MoS2 (C–MoS2) nanosheets display an unprecedented overpotential of 45 mV at 10 mA cm−2 in alkaline condition, which represents the best alkaline HER activity among the ever-reported MoS2-based catalysts. X-ray photoelectron spectroscopy (XPS) and X-ray absorption spectroscopy (XAS) systematically reveal the structural and electronic evolution of MoS2 after carbon doping. Moreover, density functional theory (DFT) analysis indicates carbon doping can generate empty p orbitals perpendicular to the basal plane of MoS2 for water adsorption and dissociation, which is essential for the alkaline HER catalysis. More importantly, the capability to endow materials with the properties which are not readily available in nature by rational orbital modulation offers a new vision for the design of HER catalysts and beyond.


Synthesis and structural characterization of C–MoS2

C–MoS2 and MoS2 were synthesized via a controlled sulfurization of Mo2C, which is illustrated in Fig. 2a. Mo2C as the precursor was obtained by a previously developed method (details, see Methods)38. Then, the as-synthesized Mo2C was controllably sulfurized to C–MoS2 and MoS2 in a home-built tube furnace with sulfur powder as the sulfur source and argon as the carrier gas (details, see Methods). The synthesized Mo2C, C–MoS2, and MoS2 were further characterized by field-emission scanning electron microscopy (SEM), X-ray diffraction (XRD), Raman spectrum, and transmission electron microscopy (TEM), respectively. SEM images in Supplementary Fig. 1 indicate the carbon fibers of the carbon cloth (CC) substrate are uniformly coated with porous Mo2C thin film, which becomes rougher after sulfurization treatment. XRD patterns (Fig. 2b) clearly reveal the Mo2C (JCPDS No. 00-035-0787) can be well converted to hexagonal MoS2 (JCPDS No. 01-073-1508) after controlled sulfurization treatment. The sharp diffraction feature of MoS2 with deep sulfurization suggests improved crystallinity. In addition, the sulfurization process can also be revealed by Raman spectroscopy (Supplementary Fig. 2). The fingerprint bands of Mo2C located at 662.5, 816.4, and 991.8 cm−1 disappear after sulfurization treatment39; meanwhile, new bands centered at around 376 and 402 cm−1 emerge, which can be assigned to the in-plane (E2g) and out-plane (A1g) Mo–S phonon mode vibration of MoS2, respectively40. Moreover, the wavenumbers of E2g and A1g of C–MoS2 display a positive shift relative to the MoS2, probably due to the susceptibility of electron–phonon coupling induced by carbon doping41,42. Taken together, all these results illustrate sulfurization treatment can well control the conversion from Mo2C to MoS2.

Fig. 2

Synthesis and characterization of C–MoS2 nanosheets. a The schematic illustration of the synthesis of C–MoS2 and MoS2. b The XRD patterns of Mo2C, C–MoS2, and MoS2. c The HRTEM image of C–MoS2. The scale bar is 10 nm. d The TEM image and the corresponding element mapping images of C, Mo, and S elements in C–MoS2. The scale bar is 200 nm

Furthermore, TEM was employed to acquire the microstructural features of Mo2C, C–MoS2, and MoS2, as shown in Supplementary Fig. 3 and Fig. 2c. The high-resolution TEM (HRTEM) images exhibit well-resolved lattice fringes, where the interplanar spacing of 0.23 nm is assigned to the (101) plane of Mo2C and 0.62 nm is assigned to the (002) plane of MoS2, respectively. Interestingly, both C–MoS2 and MoS2 prepared by sulfurization treatment are composed of ultrathin layered MoS2 nanosheets. It is also worth mentioning that no obvious carbon coating is observed on the surfaces of Mo2C, C–MoS2, and MoS2 (Supplementary Fig. 2 and Fig. 2c), offering an ideal platform to probe the intrinsic effects of carbon dopants on the properties of MoS2. In addition, the TEM image and the corresponding energy-dispersive X-ray spectroscopy (EDX) mapping images of C–MoS2 reveal homogeneous elemental distribution of C, Mo, and S elements in C–MoS2 (Fig. 2d), also suggesting possible carbon doping in the MoS2.

Chemical states and coordination structures of C–MoS2

Given that EDX spectroscopy only provides composition information that is not convincing enough to prove carbon doping into MoS2, XPS, and XAS are further used to probe localized electronic states and coordination structures of C–MoS2. Figure 3a shows the XPS Mo 3d spectra of Mo2C, MoS2, and C–MoS2, respectively. Obviously, the typical characteristics of Mo–C bonds are observed at 231.1 and 228.0 eV in Mo2C, while a pair of new peaks located at 232.6 and 229.5 eV appear after deep sulfurization, which can be assigned to the Mo 3d3/2 and Mo 3d5/2 of Mo–S bond in MoS2, respectively43. Strikingly, the Mo 3d profiles in C–MoS2 exhibit obvious shoulders at the lower binding energy region, suggesting the existence of multiple chemical states of Mo. The Mo 3d spectrum of C–MoS2 can be further deconvoluted into two pairs of peaks corresponding to the chemical states of S–Mo–S and S–Mo–C, which indicates carbon has been substitutionally doped into the MoS2 lattices (The fitting parameters are summarized in Supplementary Table 1). Meanwhile, the C 1s spectra of C–MoS2 and Mo2C (Supplementary Fig. 4, the fitting parameters in Supplementary Table 2) also support the existence of Mo–C bonds in C–MoS2. In addition, the slight shift of S 2 s position suggests the chemical environments around S atoms also slightly changes after carbon doping, which could be originated from the electronegativity difference between C and S.

Fig. 3

Chemical states and coordination structures of C–MoS2. a XPS core-level Mo 3d spectra of Mo2C, MoS2, and C–MoS2, respectively. b The normalized Mo K-edge XANES spectra. Inset: the enlarged Mo K-edge XANES spectra. c Fourier transform (FT) of Mo K-edge of Mo2C, C–MoS2, MoS2, and Mo foil. d The whole contour plots of wavelet transform (WT) of MoS2 and C–MoS2 (upper) and the more-refined first shell analysis (lower). e Radial distribution of Fourier-transformed EXAFS signal of C–MoS2

To probe the evolution of localized coordination environment in MoS2 induced by carbon doping, X-ray absorption near-edge structure (XANES) and extended X-ray absorption fine structure (EXAFS) are performed. Figure 3b shows the Mo K-edge XANES spectra of Mo2C, C–MoS2, MoS2, and Mo foil, in which Mo foil is used as the reference. Apparently, the Mo foil possesses the smallest energy of absorption edge. Moreover, the enlarged Mo K-edge XANES curves (inset, Fig. 3b) reveal that the near-edge absorption energy of C–MoS2 located between MoS2 and Mo2C indicates the average electron density around Mo in C–MoS2 is higher than MoS2 but lower than Mo2C, which is consistent to the XPS Mo 3d spectra and also suggests the existence of Mo–C bonds in C–MoS2. In addition, Mo K-edge extended XAFS oscillation functions k2χ(k) of MoS2, C–MoS2, Mo2C, and MoS2 mixed with small amounts of Mo2C (denoted as Mo2C + MoS2) are presented in Supplementary Fig. 5a, respectively. Clearly, the oscillation of C–MoS2 is very similar to MoS2, but quite different from Mo2C and Mo2C + MoS2, convincingly indicating the C–MoS2 possesses similar structure to MoS2 and there is no obvious Mo2C remaining in C–MoS2. Moreover, the XPS depth profiling analysis also does not show obvious existence of Mo2C (Supplementary Fig. 5b). Figure 3c displays the corresponding R-space curves of Mo after k2 [χ(k)] weighted Fourier transform. The shoulder peaks at around 1.9 and 2.9 Å in MoS2 are originated from the Mo–S and Mo–Mo vectors, respectively44. Considering the positions of Mo–C and Mo–O are very close and no obvious Mo–O states are observed in the XPS Mo 3d spectra, we reasonably believe the peak at 1.3 Å in C–MoS2 could be assigned to the Mo–C bond45. To more clearly reveal the coordination structures in C–MoS2, wavelet transform (WT) with high resolution in both k and R spaces of Mo K-edge EXAFS oscillation are further performed. The whole WT contour spectra are shown in the Fig. 3d (the upper). The intensity maxima at R = 1.9 and 2.9 Å are attributed to the Mo–S and Mo–Mo bonds, respectively. Owing to the small bond length difference between Mo–C and Mo–S, more-refined first shell analysis of MoS2 and C–MoS2 is further carried out (Fig. 3d, the lower). Apparently, MoS2 possesses only one contour centered at about k = 5.4 Å−1, originated from the Mo–S bond, while C–MoS2 presents one more maximum intensity at k = 4.6 Å−1, which is very close to the Mo–C in Mo2C centered at about k = 4.5 Å−1 (Supplementary Fig. 6a) and far from the Mo–O in MoO2 with the maximum intensity at k = 6.0 Å−1 (Supplementary Fig. 6b), and thus can be well assigned to the Mo–C. Meanwhile, we also conduct the EXAFS fitting in the range of 1.1 to 2.3 Å by using the Mo–O and Mo–C path at 1.3 Å, respectively (Supplementary Fig. 6c,d). Based on the fitting parameters presented in the Supplementary Table 3, the Rf value for the Mo–O model (2.9%) is much larger than that of the Mo–C path (1.1%), further suggesting the Mo–C path is more likely than the Mo–O path in the C–MoS2. In light of the formation of Mo–C in C–MoS2, the coordination environment of MoS2 may also alter with carbon doping. Furthermore, the EXAFS data of MoS2 and C–MoS2 are fitted through the Artemis to get detailed structural parameters (Supplementary Fig. 7 and Fig. 3e). The coordination number of Mo–S is fitted to be around 6 for the MoS2, while the coordination number of Mo–S is deceased to 4.8 and the coordination number of Mo–C is 1.1 in the C–MoS2. The detailed fitting parameters are summarized in Supplementary Table 4. Although we cannot exclude the existence of Mo2C clusters in C–MoS2 that is beyond the detection limits of the currently used characterization techniques, our experimental results clearly reveal that carbon is most probably doped into the lattices of MoS2 in the form of Mo–C bond.

Alkaline hydrogen evolution catalysis of C–MoS2

The alkaline HER catalysis is evaluated in 1.0 M KOH solution using a typical three-electrode system with the studied materials as the working electrodes, Hg/HgO as the reference electrode and graphite rod as the counter electrode. Figure 4a shows the linear sweep voltammetry (LSV) curves of CC, Mo2C, C–MoS2, MoS2, and Pt/C with a scan rate of 5 mV s−1, in which the blank CC and benchmark Pt/C are used as control samples. Impressively, C–MoS2 delivers higher current density and lower current onset potential than CC, MoS2, and Mo2C, indicating carbon doping can substantially improve the catalytic performance toward HER in alkaline condition. Carbon doping enables the overpotential of C–MoS2 at 10 mA cm−2 to be as low as 45 mV, which is much better than the 200 mV of Mo2C and 228 mV of MoS2 and even close to the catalytic activity of Pt/C (30 mV). Although the performance of C–MoS2 is not the best among all kinds of the HER catalysts including non-precious and precious catalysts, C–MoS2 represents the best alkaline HER activity among the ever-reported MoS2 (Fig. 4b and Supplementary Table 5 and 6)7,19,32,33,34,36,37,46,47,48, which could provide valuable insights for the active site engineering. The faradaic efficiency of the C–MoS2 for HER catalysis is estimated to be around 97%. Given that temperature can well control the sulfurization degrees, we also study the sulfurization degree-dependent HER activities (Supplementary Fig. 8). With the increase of the sulfurization temperatures, the HER overpotentials display an inverse volcano-shaped feature. At the temperature below 500 °C, Mo2C cannot be completely converted to MoS2 and the corresponding catalytic activity is far less than that of the C–MoS2, further revealing C doping probably plays vital role in the HER catalysis. To probe the effects of carbon contents, we further study the carbon content dependent HER activities of C–MoS2 (Supplementary Fig. 9). Obviously, with the increase of carbon concentration, the catalytic activity of C–MoS2 increases and reaches a maximum value. However, further increasing the C ratio will result in performance decay probably due to too much destroy of the layered structures of MoS2, suggesting moderate carbon doping in MoS2 is essential for the HER catalysis. Additionally, Tafel slope can be used to probe the effects of carbon dopants on the rate-determining steps during HER process. Figure 4c displays the corresponding Tafel curves. The derived Tafel slope of MoS2 is around 129 mV dec−1, suggesting the alkaline HER catalysis on MoS2 undergoes Volmer mechanism and water dissociation is the rate-determining step. Importantly, C–MoS2 exhibits a substantially decreased Tafel slope of 46 mV dec−1, clearly revealing the sluggish water dissociation behavior has been significantly improved after carbon doping. Meanwhile, the exchange current densities for Mo2C, MoS2, C–MoS2, and Pt/C derived by Tafel extrapolation are 0.12, 0.25, 0.87, and 1.28 mA cm−2, respectively. Clearly, although the exchange current density of C–MoS2 is a little smaller than that of Pt, it is still substantially larger than that of MoS2, also suggesting carbon doping can change the intrinsic catalytic activities of MoS2 for alkaline HER catalysis.

Fig. 4

Alkaline HER catalysis of C–MoS2. a The LSV curves of CC, Mo2C, C–MoS2, MoS2, and Pt/C with IR correction. b Performance comparison of C–MoS2 with the ever-reported MoS2-based catalysts in alkaline condition. c The corresponding Tafel slopes. d The potential-dependent TOF curves of Mo2C, MoS2, and C–MoS2. e Nyquist plots of Mo2C, MoS2, and C–MoS2 collected at the potential of 100 mV vs. RHE. f The initial and 1000th polarization curves of C–MoS2. The inset is the chronoamperometric curve recorded at −0.1 V vs. RHE without IR correction for a continuous 240 h

Considering surface area may also affect the HER catalytic performance, we further estimate the electrochemical surface areas of the studied materials by deriving the electrochemical double layer capacitance (Cdl) from the cyclic voltammetry studies (Supplementary Fig. 10)11. The C–MoS2 is found to have a larger Cdl of 54 mF cm−2 than MoS2 (19 mF cm−2) and Mo2C (27 mF cm−2), indicating carbon doping treatment can also increase the surface area of C–MoS2. To eliminate the influence of surface area and reveal the intrinsic catalytic behavior, turnover frequency (TOF), a surface area independent figure of merit, is calculated to gain the intrinsic per-site activity, as shown in Fig. 4d. Impressively, the TOF values of C–MoS2 are significantly larger than those of MoS2 and Mo2C, clearly revealing carbon doping can essentially promote the per-site activity for HER catalysis. Additionally, electrochemical impedance spectroscopy (EIS) in Fig. 4e presents that C–MoS2 possesses a smaller charge transfer resistance (Rct) of 32.1 Ω than MoS2 (83.7 Ω) and Mo2C (59.7 Ω), further suggesting carbon doping in MoS2 can also substantially boost the interfacial electron-transfer kinetics. Besides carbon doping, the superior electrochemical behavior of C–MoS2 is also attributed to the unique carbon doping strategy without involving carbon deposition on the catalyst surface. We also use a conventional post-doping method to introduce carbon and study their electrochemical performance, shown in Supplementary Fig. 11. TEM image clearly illustrates obvious carbon shell deposited on the surface of MoS2, which results in decreased catalytic performance probably due to the blocked active sites for catalysis (Supplementary Fig. 12). Given that the MoS2 is derived from Mo2C which may have tiny amounts of carbon remaining, MoS2 with minimum carbon interference is also prepared by thermal sulfurization of ammonium molybdate (Supplementary Fig. 13). Electrochemical studies reveal that the HER performance of the newly prepared MoS2 is far less than that of C–MoS2, also suggesting carbon dopants play vital roles in the HER catalysis of C–MoS2. Finally, the stability of C–MoS2 is evaluated by polarization cycling and chronoamperometric test, both of which display superior catalytic stability for alkaline electrolysis (Fig. 4f). XPS and XAFS are further employed to evaluate the C–MoS2 after the stability test (Supplementary Fig. 14). Impressively, there is no big difference in chemical and bonding states in C–MoS2 before and after the durability test, suggesting the robustness of the C–MoS2 for HER catalysis.


To decipher the modulation essence of the carbon dopants in C–MoS2 for alkaline HER catalysis at the atomic level, DFT calculations are further carried out. The C content used in the C–MoS2 model is based on the area ratio of Mo–C and Mo–S states in the XPS Mo 3d of C–MoS2. In light of the charge balance after carbon doping, we also introduce sulfur vacancies (Vs) in the structural models. To equally distribute the positions of the C dopants and S vacancies, we considered seven different configurations, as shown in Supplementary Fig. 15. Supplementary Fig. 16 shows one of the typical structures of C–MoS2, where the C dopants are pulled into the sublayer of MoS2, due to the formed stronger Mo–C bond with shorter bond length than the original Mo–S bond. Detailed bond length information is provided in Supplementary Fig. 17. The electron density difference images in Supplementary Figs 18 and 19 clearly reveal that the introduction of carbon can significantly break the unified surface electron distribution of MoS2. More importantly, the orbital analysis in Fig. 5a and b indicates the carbon dopants prefer to form the sp2 hybrid orbitals (highlighted by red dash circle in Fig. 5a), which thus vacates an unhybridized 2pz orbital perpendicular to the basal plane (highlighted by red dash circle in Fig. 5b). This 2pz orbital orientation can maximize the head-on orbital overlapping to form sigma bonds, which can potentially offer active sites for water adsorption and activation. This orbital orientation is also consistently observed on the other structural configurations of C–MoS2, as shown in Supplementary Fig. 15. Additionally, the detailed partial density of states (PDOS) analysis (Supplementary Fig. 20) indicates that carbon doping can well increase the electrical conductivity of the MoS2 and thus could benefit the electron transportation and enhance the catalytic activity. Although conductivity is important for electrocatalysis, we reasonably believe the exceptional alkaline HER activity of C–MoS2 is mainly stemmed from the C-induced orbital tuning for water adsorption and dissociation, considering 1-T MoS2 with better conductivity does not exhibit such exceptional activity49. Moreover, the electrostatic potential mapping images (Fig. 5c and Supplementary Fig. 21) and the electron density difference slices (Supplementary Fig. 22) further reveal superior water adsorption on the basal plane of C–MoS2, which is confirmed by the apparent charge transfer and the formation of remarkable chemical bonding orbital between water and C–MoS2 (Fig. 5c), while no apparent orbital bonding or charge interaction occurs on MoS2 (Fig. 5d). We also consider the MoS2 model with only sulfur vacancies. Structural analysis indicates sulfur vacancies indeed do not have obvious effects on the orbital orientation tuning (Supplementary Fig. 23a). The corresponding water adsorption energy on the defected MoS2 (MoS2-Vs) is around −0.23 eV, which is only slightly higher than that on the MoS2. Meanwhile, we also experimentally prepare MoS2 with sulfur vacancies via a typical hydrogen treatment and study their electrochemical properties. The overall performance of the hydrogen treated MoS2 is still far less than that of C–MoS2 (Supplementary Fig. 23b), suggesting the sulfur vacancy may not be the main factor for the exceptional alkaline HER activity of the C–MoS2. Taken together, all the structural information consistently suggest that carbon doping can effectively manipulate the orbital orientation and create more active sites on the basal plane of MoS2 for water adsorption and activation.

Fig. 5

The structural analysis and the catalytic pathway of C–MoS2. The top-view and side-view sp2 hybrid orbitals (highlighted by red dash circle) at the top of valence band (a) and the empty 2p orbitals (highlighted by red dash circle) perpendicular to the basal plane at the bottom of conduction band (b) of C–MoS2. The top-view electrostatic potential of water adsorbed on the basal plane of C–MoS2 (c) and MoS2 (d) and the corresponding side-view bonding and non-bonding orbitals. e The relative energy diagram along the reaction coordinate, including the first (left panel) and second (right panel) water dissociation process on the basal plane of MoS2 and C–MoS2, respectively. R reactant, RC reactant complex, TS transition state, IM intermediate

Besides structural information, alkaline HER catalytic pathways on the basal plane of MoS2 and C–MoS2 are further studied. Figure 5e shows the relative energy profiles of water adsorption and dissociation on MoS2 and C–MoS2, respectively. As expected, the basal plane of MoS2 is almost inert for alkaline HER catalysis, with poor water adsorption and giant water dissociation energy barrier. Impressively, carbon doping enables the HER catalysis to proceed on a much lower potential energy surface. Specifically, C–MoS2 owns more favorable adsorption energies (−0.53 eV for RC1 & −0.25 eV for RC2) and much lower transition state energy barrier (0.70 eV for TS1 & 1.15 eV for TS2). From the water adsorption/dissociation configurations on C–MoS2 (Fig. 5e), H2O is adsorbed on the C site, while the nearby S sites assist water dissociation by attracting the H in water molecule. In addition, we also performed the catalytic pathway of Mo2C (001) (Supplementary Fig. 24). Obviously, the reaction on the Mo2C proceeds on a potential energy surface with much higher energy barrier than that on C–MoS2. Moreover, the generated hydrogen adsorbed intermediate (Sur-H) is so stable that the adsorbed hydrogen needs overcome 1.37 eV for H desorption from the carbon site of the surface, which could potentially impede the HER catalysis. The studies on the catalytic pathways clearly reveal carbon doping could intrinsically boost the water adsorption and dissociation kinetics and thus endow MoS2 with exceptional alkaline catalysis by tuning the orbital orientations on the basal plane.

In summary, we have demonstrated carbon doping can intrinsically endow MoS2 with exceptional alkaline HER catalytic capability by tuning the orbital orientation. In comparison with the inert alkaline HER activity of MoS2, the prepared C–MoS2 achieves an overpotential of 45 mV at 10 mA cm−2, which is very close to the commercial Pt/C and also represents the best catalytic activity among the ever-reported MoS2 for alkaline HER catalysis. XPS and XAS analysis reveal that the electronic and coordination structures of MoS2 have been significantly changed after carbon doping. DFT studies further indicate that carbon-induced empty 2p orbitals perpendicular to the basal plane of MoS2 enable energetically favorable water adsorption and dissociation, and thus promote the alkaline HER catalytic kinetics. The capability to intrinsically manipulate the catalytic activities by orbital modulation could offer a powerful platform to rationally design HER catalysts and beyond.


Reagents and chemicals

Ammonium molybdate ((NH4)6Mo7O24·4H2O), Potassium hydroxide, Cetyltrimethyl ammonium bromide (CTAB), Thiourea and Sublimed sulfur were purchased from Shanghai Sinopharm Chemical Reagent Co., Ltd. CC was purchased from Shanghai Hesen Electric Co., Ltd.

Synthesis of Mo2C

Typically, 3.708 g ammonium molybdate and 1.638 g CTAB were dissolved in 30 mL and 180 mL deionized water with ultrasonic assistance, respectively. Then, the two solutions were mixed homogeneously by magnetically stirring for 30 min, and further aged for another 24 h to obtain a uniform emulsion. A volume of 15 mL of the as-prepared emulsion was transferred into a 20 mL Teflon-lined stainless steel autoclave with the pretreated CC (CC, 2*3 cm2, pretreated with nitric acid and deionized water, respectively) as the growth substrate. After keeping the autoclave at 200 °C for 20 h, the CC was taken out, cleaned by deionized water and dried at vacuum oven at 60 °C overnight. Finally, Mo2C was obtained by annealing the prepared samples at 900 °C for 6 h in a home-built tube furnace system under argon atmosphere.

Synthesis of C–MoS2 and MoS2

C–MoS2 and MoS2 were prepared by a temperature-controlled sulfurization process. The as-prepared Mo2C was sulfurized in a tube furnace system for 2 h with powdered sulfur as the sulfur source and argon as the carrier gas (flowing rate at 20 sccm). The sulfurization temperatures can be tuned from 500 to 900 °C. The optimized C–MoS2 was achieved at 600 °C with a partial sulfurization, while MoS2 was fabricated at 900 °C with a deep sulfurization. As comparison, a post-doping strategy was employed to dope carbon into MoS2. The carbon doped MoS2 by post-doping method (PC–MoS2) was achieved by annealing MoS2 at 750 °C for 0.5 h under acetylene flow. MoS2 with minimum carbon interference was synthesized by sulfurizing ammonium molybdate with S as the sulfur source and argon as the carrier gas (flowing rate at 20 sccm) for 2.0 h under 900 °C25.

Structural characterizations

XRD measurements were performed on a Philips X’Pert Pro Super diffractometer using Cu Kα radiation (λ = 1.54178 Å). The field-emission scanning (FE-SEM) images were collected using a FEI Sirion-200 SEM, while TEM and HRTEM images were acquired at a JEOL-2010 TEM with an acceleration voltage of 200 kV. Raman spectra were recorded on a Renishaw RM 3000 Micro-Raman system. XPS were performed at the photoemission end-station (BL10B) in the National Synchrotron Radiation Laboratory (NSRL), Hefei. To avoid the carbon interference for the binding energy calibration, all the samples were sprayed with tiny amount of Au as an external standard and the obtained binding energies were calibrated using the Au 4f energy (Au 4f7/2, binding energy of 84 eV). The XPS fitting was performed using the XPS PEAK41 software with Shirley background subtraction. The XPS database (NIST X-ray Photoelectron Spectroscopy Database, was used as a reference to assign the possible chemical states. During fitting, the peak intensity ratio and the full width at half maximum (FWHM) were well constrained in a reasonable range. XAS measurements were conducted at the beamline (BL14W1) of Shanghai National Synchrotron Radiation Facility (SSRF, China). The EXAFS data were disposed according to the standard procedures through the ATHENA module implemented in the IFEFFIT software packages50. The quantitative curve-fittings were conducted for the Fourier-transformed k2-weighted χ(k) in the R-space with a Fourier transform k-space range of 3.1–11 Å−1 by employing the module ARTEMIS 4 of IFEFFIT. The backscattering amplitude F(k) and phase shift Φ(k) were calculated by FEFF8.0 code. While the curve-fitting, all the amplitude reduction factor S02 was set to the best-fit value of 0.85 determined from fitting the data of MoS2. In order to fit the curves in the R-range of 1.1–3.4 Å, we considered Mo–C, Mo–Mo and Mo–S paths as the central-peripheral. For each path, the structural parameters, like coordination number (N), interatomic distance (R), and edge-energy shift (ΔE0) were opened to be varied. For the Mo–C, Mo–S, and Mo–Mo coordination, the common adjustable parameters of ΔE0 and σ2 were employed to reduce the number of free parameters.

Electrochemical measurements

All the electrochemical characterizations were performed in a three-electrode system on CHI 760E electrochemical workstation. The studied materials grown on CC were used as working electrodes, while Hg/HgO electrode and graphite rod were employed as the reference and counter electrodes, respectively. All the measurements were conducted in 1.0 M KOH electrolyte and the potentials vs. Hg/HgO were converted with respect to the reversible hydrogen electrode (RHE) using the equation E (vs. RHE) = E (vs. Hg/HgO) + E0 (Hg/HgO) + 0.059*pH in the 1.0 M KOH. LSV curves were collected with a scan rate of 5 mV s−1 and the LSV curves shown in the manuscript were corrected by IR compensation (EiR-corrected = Eoriginal – I * Rs). The chronoamperometry curve was performed for the durability test at the potential of −0.1 V vs. RHE. Electrochemical surface area (ECSA) was obtained by conducting cyclic voltammetry (CV) in the range of 0.1–0.2 V vs. RHE with various scan rates from 10 to 50 mV s−1. The current density differences (Δj = ja − jc) were plotted against scan rates, and the slopes can be used to derive Cdl and the ECSA. EIS measurements were carried out at the potential of −0.1 V (vs. RHE) in the frequency range of 100,000–0.001 Hz with a perturbation of 5 mV. TOF values were calculated using a previously reported method, in which the number of active sites was estimated as the amount of surface sites (including C, Mo, and S atoms)11. The Faradic efficiency of C–MoS2 was evaluated in a H-type cell with an anion exchange membrane as the separator and 20 mL 1.0 M KOH as the electrolyte in each compartment, with a gas chromatography (HA GC-9560) for the hydrogen gas detection. The gas production was detected by the gas chromatography and the Faradic efficiency was calculated using the formula: Faradic efficiency = 2 F × \({\mathrm{N}}_{{\mathrm{H}}_2}\)/Q = 2 F × \({\mathrm{N}}_{{\mathrm{H}}_2}\)/(It), where F is the Faradic constant, I is the current, t is the running time and \({\mathrm{N}}_{{\mathrm{H}}_2}\) is the amount of H2 production.

Density functional theory calculation

All the DFT calculations were carried out using the CASTEP program in Material Studio package of Accelrys Inc51. The exchange-correlation functional was employed by the Perdew-Burke-Ernzerhof (PBE) of generalized gradient approximation (GGA) with the ultrasoft pseudopotentials (USP). The van der Walls interactions was considered by the DFT dispersion correction (DFT-D). The number of plane wave was determined by an energy cutoff of 450 eV. The Brillouin zone was sampled by a 2 × 2 × 1 k-points grid for the structure optimizations and double k-points meshes were employed for the density of states (DOS) calculations, respectively. A complete linear synchronous transitions (LST) and quadratic synchronous transitions (QST) approach was used for the transition state searching. The convergence tolerances were set to 2.0 * 10−6 eV per atom for energy, 0.002 Å for maximum displacement, and 0.05 eV Å−1 for maximum force. The surfaces were modeled by a periodic slab repeated in 6 * \(\sqrt 2\) * 2 \(\sqrt 2\) surface unit cell with a vacuum region of 13 Å between the slabs along the z axis. The H2O absorption energy was calculated using the following equation, \({\mathrm{\Delta E}}_{{\mathrm{H}}_2{\mathrm{O}}} = {\mathrm{E}}_{{\mathrm{surf}} - {\mathrm{H}}_2{\mathrm{O}}} - {\mathrm{E}}_{{\mathrm{surf}}} - {\mathrm{E}}_{{\mathrm{H}}_2{\mathrm{O}}}\), where \({\mathrm{E}}_{{\mathrm{surf}} - {\mathrm{H}}_2{\mathrm{O}}}\) and Esurf are the total energies of the surface covered with and without H2O molecule, \({\mathrm{E}}_{{\mathrm{H}}_2{\mathrm{O}}}\) is the energy of free H2O molecule.

Data availability

The authors declare that the main data to support the finds of this study are available within the article and its Supplementary Information. Extra data are available from the corresponding author upon request


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We thank the financial support of the National Key Research and Development Program of China (2017YFA0206703), Natural Science Fund of China (No. 21771169, 11722543, 11505187), the Fundamental Research Funds for the Central Universities (WK2060190074, WK2060190081, and WK2310000066), USTC start-up funding, and Recruitment Program of Global Expert. We also acknowledge the beamline BL10B at National Synchrotron Radiation Laboratory, and the Beamline BL14W1 at Shanghai Synchrotron Radiation Facility for XPS and XAFS characterizations. The numerical calculations in this paper have been done on the supercomputing system in the Supercomputing Center of University of Science and Technology of China.

Author information

G.W. and Y.Q. designed and supervised the project. Y.Z. and S.N. conducted the project and contributed equally to this work. J.Y., Y.W., X.Z. and J.Zhu conducted XPS and XAS measurements. J.C., Y.X., Y.L. and J.Z. performed SEM and TEM characterization. X.L. and S.N. provided the DFT calculation. G.W., Y.Z. and X.L. wrote and revised the manuscript, and all the authors discussed the results and commented on the manuscript.

Correspondence to Xiaojing Liu or Gongming Wang.

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