Xianglong
Meng‡
a,
Hailing
Guo‡
*a,
Kun
Sun
a,
Xuyu
Zhao
a,
Girolamo
Giordano
b,
Yongming
Chai
a and
Chenguang
Liu
a
aState Key Laboratory of Heavy Oil Processing, Key Laboratory of Catalysis, China National Petroleum Corp., China University of Petroleum (East China), Qingdao 266555, PR China. E-mail: guohl@upc.edu.cn
bC.E.Ca.S.P. Laboratory, University of Calabria, Rende 87036, Italy
First published on 9th October 2025
The MoS2 catalyst shows great potential in deep hydrodesulfurization (HDS) but is limited by high metal usage and low active site utilization. A MoS2–GO composite catalyst with trace amounts of graphene oxide (GO) was synthesized via an in situ solvothermal method. Owing to its high polarity, deionized water acts as an effective dispersant for GO, ensuring uniform dispersion while preserving its sheet-like morphology. The Mo precursor, bearing organic functional groups, is homogeneously anchored onto the oxygen functionalities of GO sheets, resulting in a densely packed monolayer MoS2 structure with abundant, highly exposed HDS edge sites across the layered GO surface. Combined X-ray photoelectron spectroscopy (XPS) and density functional theory (DFT) analyses reveal that MoS2 forms a heterostructure with GO through interactions between S atoms and the surface oxygen functionalities of GO. In the HDS reaction, it achieves 98.3% dibenzothiophene (DBT) conversion at 280 °C and exhibits high hydrogenation desulfurization (HYD) selectivity (S(HYD/DDS) up to 12.8). Notably, it demonstrates excellent activity for sterically hindered 4,6-dimethyldibenzothiophene (4,6-DMDBT, 80.7% conversion at 300 °C) and a high HYD pathway selectivity (S(HYD/DDS) up to 13.9). Raman spectroscopy coupled with DFT calculations reveals that the MoS2–GO catalyst features extensive Mo–S–O(GO) electron-transport networks, which facilitate H2 dissociation and drive continuous hydrodesulfurization of sulfur-containing species. This study provides insights into the preparation of heavy oil hydrocracking catalysts and the regulation of hydrogenation pathway selectivity.
Non-supported catalysts, owing to their high active component content, are considered to have enormous potential for hydrogenation desulfurization.6,8 In particular, non-supported MoS2 catalysts exhibit superior HYD/DDS selectivity, distinguishing them from the other deep hydrogenation desulfurization catalysts and aligning with emerging hydrogenation requirements.9–11 Based on the “rim-edge” model proposed by Daage and Chianelli,12 it has been suggested that the edge sites of MoS2 stacks—specifically those on the top and bottom layers—participate in both the HYD and DDS pathways, while the edge sites in the intermediate layers predominantly favor the DDS pathway. The active sites for HDS, also referred to as S vacancies, may be located at either the Mo edge or the S edge of molybdenum-based catalysts.13–15 Strategies for optimizing the performance of unsupported MoS2 catalysts involve not only tailoring the relative proportions of different active sites but also engineering structures with highly exposed active sites to maximize the utilization efficiency of active metals.
The low active metal utilization is a critical factor limiting the performance enhancement and large-scale industrialization of MoS2 catalysts, and it has long been a primary focus of research.16 Currently, researchers often employ strategies such as constructing porous or layered structures to achieve high exposure of active metals. This involves adding templates or structure-directing agents during synthesis. For example, some researchers have used mesoporous carbon,17 carbon nitride,18 and silica19 as templates to synthesize porous Mo-based catalysts via hydrothermal methods, significantly enhancing catalyst activity. Wang et al. selected nickel–aluminum layered double hydroxide (NiAl-LDH) as a structure-directing template to synthesize a multimetallic NiAlMoW catalyst.20 This catalyst exhibits intrinsic catalytic activity twice that of commercial CoNiMoW/Al2O3 catalysts. Although methods to optimize MoS2 catalyst structures can enhance the atomic utilization of non-supported molybdenum-based catalysts to some extent, they are not easy to develop. The use of templates necessitates their removal—often with strong acids or bases—which may lead to pore collapse during subsequent sulfidation or calcination, resulting in poor catalyst stability.17–20 Secondly, although porous or layered structures can fully expose active sites, the selectivity of desulfurization pathways has not been effectively regulated.19,20 Therefore, further investigation into microscale structures remains a key research focus.
Building on our previous research, single-layer MoS2 nanosheets have been successfully synthesized using organic solvents, enhancing the utilization of active sites and mass transfer efficiency.21 Further optimization of the desulfurization activity and pathway selectivity of unsupported MoS2 catalysts is required. Under solvothermal conditions, non-metallic additives can be introduced in situ to further modulate the microstructure and morphology of non-supported MoS2, thereby increasing the abundance of MoS2 edge sites and enhancing metal utilization. Evidence from previous studies indicates that oxygen-containing groups on GO readily anchor and couple with Mo precursors bearing organic groups in organic media, thereby ensuring high dispersion of Mo precursors.22–24 However, for MoS2–GO composites, the key challenge is that this two-dimensional material tends to aggregate or tightly stack during the composite process due to van der Waals forces or strong π–π interactions.25,26 This leads to reduced dispersion, surface area, and GO defect sites, thereby limiting the improvement of catalytic activity in the composite material. Therefore, achieving the dispersion of GO in the synthesis solution and the anchoring and uniform dispersion of MoS2 on GO sheets has emerged as a key research focus.
In this study, MoS2–GO composite sheet cluster catalysts were synthesized by the in situ solvothermal method. GO readily exfoliates into single sheets in highly polar deionized water. Its abundant surface oxygen functionalities anchor Mo-based organic precursors, enabling this method to successfully achieve the effective dispersion and oriented alignment of monolayer MoS2 on GO sheets. In the HDS reaction, it achieves 98.3% dibenzothiophene (DBT) conversion at 280 °C and exhibits high HYD desulfurization selectivity (S(HYD/DDS) up to 12.8). The HYD pathway exhibits selectivity 7 times higher than that of solvothermally synthesized MoS2 catalysts and 6 times higher than that of the ethanol-dispersed MoGO-E catalyst. Notably, it demonstrates excellent activity for sterically hindered 4,6-dimethyldibenzothiophene (4,6-DMDBT, 80.7% conversion at 300 °C) and a high HYD pathway selectivity (S(HYD/DDS) up to 13.9). The integration of Mo–S–O(GO) electron-transfer pathways with GO defect sites constructs a robust interfacial network that promotes H2 activation and selectively enhances the HYD route.
This work is a classic case of engineering precision control of hydrogenation desulfurization MoS2 catalysts to achieve high activity, high selectivity, and high stability catalyst utilization.
Using an identical synthesis procedure and the same molybdenum precursor dosage, MoS2–GO composite catalysts were prepared with GO doping amounts of 1 g, 1.5 g, and 2.5 g, respectively; in each case, the GO (0.94 wt%) was dispersed in 2 mL of deionized water. The catalysts were designated as MoGO1, MoGO1.5, MoGO2 (MoGO-W) and MoGO2.5 according to the GO doping level.
The average slab length
and the average number of stacked layers
were statistically calculated by HRTEM images according to the following formula.21
![]() | (1) |
N i is the stacking number of the layers, and ni is the number of stacked units with a stacking number of Ni.20
![]() | (2) |
L i is the length of the layer, and ni represents the number of layers with a length Li.
DFT calculations were performed with the Vienna Ab Initio Simulation Package (VASP) using spin-polarized GGA–PBE.27 The PAW method and a plane-wave cutoff of 400 eV were employed. Geometry optimizations used a force convergence criterion of 0.03 eV Å−1 and an SCF energy threshold of 1 × 10−4 Ha, with a 1 × 1 × 1 k-point mesh. Slab models comprised a three-layer GO sheet (derived from graphene (001)) and the MoS2 (002) plane, each represented by p (3 × 3) supercells and separated by a 15 Å vacuum. Three models—MoS2-1Layer, MoS2–GO and MoS2-2Layer—were constructed to evaluate the adsorption energies and Gibbs free energies.
The adsorption energy (Eads) of hydrogen molecules on the surface is calculated using the following equation (eqn (3)):15,27
| Eads = E(adsorbate+surface) − Esurface − Egas | (3) |
In this equation, Esurface represents the total energy of the surface without adsorption, Egas is the energy of the free gas molecules in the vacuum, and Eadsorbats+surface is the total energy of the system after adsorption. A negative value of Eads indicates that the process is exothermic, and adsorption can occur spontaneously. An example of this application is reported in SI.
The main products of the DBT HDS reaction are biphenyl (BP), cyclohexylbenzene (CHB), and bicyclohexyl (BCH). Biphenyl is primarily produced via the DDS pathway, while BP and CHB are generated through the HYD pathway. The selectivity of the HYD pathway can be obtained using21
![]() | (4) |
In this equation, CBP, CCHB, and CBCH represent the concentrations of BP, CHB, and BCH in the reaction products, respectively.
To compare the activity per unit mass of the catalysts, the activation energy (Ea) of the HDS of DBT and 4,6-DMDBT over all the catalysts was calculated according to the Arrhenius formula. At each temperature, the apparent rate constant was first calculated from the experimental conversion based on the reaction order. Since the desulfurization reaction with sulfides (DBT or 4,6-DMDBT) can be approximated as a first-order process, the integrated rate equation:
| X = 1 − e−kt | (5) |
The formula:
![]() | (6) |
Here, X denotes the conversion of DBT or 4,6-DMDBT in HDS, t is the reaction time, k refers to the rate constant of DBT or 4,6-DMDBT in HDS (mol g−1 h−1), T refers to the reaction temperature (K), R refers to the gas constant (8.314), and C refers to the constant.
Due to the incorporation of GO, all the MoS2–GO catalysts exhibited a Mo loading of approximately 36 wt%, which is lower than the 47.9 wt% observed for Solvo-MoS2. MoGO-W exhibits high dispersion and the lowest specific surface area (<13 m2 g−1, Fig. S1 and Table S1), indicating effective suppression of MoS2 nanosheet stacking and the formation of additional intercrystalline mesopores.27,28 The GO composite had no significant effect on the phase composition or crystallization of Solvo-MoS2 (Fig. 1a). From the infrared spectra, it can be observed that the solvothermal series catalysts (MoGO and Solvo-MoS2) exhibited saturated C–H bond stretching vibration peaks at 2858 cm−1 and 2930 cm−1, indicating the presence of organic compounds (Fig. 1b).21,28 Thermogravimetric analysis further confirms that the weight loss primarily arises from the release of organic species (Fig. S2). After GO incorporation, the MoGO-W and MoGO-E catalysts showed vibration peaks at 1101 cm−1, 1220 cm−1, and 1618 cm−1, which correspond to C–O–C, C–O, and C–OH bonds,25,29,30 respectively, indicating the successful incorporation of GO components.
Raman spectroscopy was used to analyze the composition and structure of the MoS2–GO catalysts. In the 200–500 cm−1 range, all three solvothermal catalysts showed Raman peaks at 234 cm−1, 280 cm−1, and 333 cm−1, corresponding to the characteristic modes of monolayer MoS2 (1T/MoS2) (Fig. 1c).31,32 The J2 and J3 peaks of the MoGO-W and MoGO-E catalysts shifted to lower wavenumbers compared to solvothermal MoS2, indicating GO incorporation.31,33 The MoGO-W and MoGO-E catalysts also displayed GO-related Raman peaks, including the D band at 1348 cm−1 (the vibrations of disordered, edge, and defect sites of sp3-hybridized carbon atoms in graphene) and the G band at 1595.9 cm−1 (the vibrations of sp3 carbon atoms in an ideal graphene layer).34,35 The ID/IG ratio was higher for MoGO-W (1.40) than for MoGO-E (1.13), indicating more defects (Fig. 1d). These results indicate the successful integration of monolayer MoS2 with GO. Furthermore, under solvothermal and thiourea-sulfurization conditions, the removal of oxygen-containing groups from GO leads to the exposure of additional defect sites.36,37
XPS analysis was performed to investigate the elemental valence states in the MoS2 catalysts doped with GO. Upon analysis, GO had no significant effect on the binding energy of Mo4+ (Fig. 2a). The Mo 3d3/2 and Mo 3d5/2 peaks for all three samples appeared near 231.5 eV and 228.3 eV, respectively, with a slight increase in the sulfurization degree of Mo (Table S2). XPS S 2p spectra of the three catalysts show that the S 2p peak of Solvo-MoS2 appears at 160.3 eV, whereas those of MoGO-W and MoGO-E shift to 161.0 and 161.4 eV, respectively, consistent with the defect sites in GO depleting the electron density around MoS2-associated S atoms and thus increasing the S 2p binding energy (Fig. 2b). Concurrently, the C 1s feature assigned to C
C/C–C shifts from 284.6 eV in Solvo-MoS2 to 284.1 eV in the MoGO samples (Fig. 2c). Together, these shifts indicate electronic interaction between MoS2 and GO and support the formation of a MoS2–GO composite.38,39
The MoGO-W catalyst retains the sheet-like morphology of graphene oxide, forming densely aligned MoS2 nanosheets on the surface (Fig. 3a). In contrast, MoGO-E, dispersed in anhydrous ethanol, exhibits spherical-like nanoparticle morphology resembling that of Solvo-MoS2 (Fig. 3b and c). The difference in the dispersion stability of GO in deionized water and ethanol primarily arises from the variation in hydrogen-bonding interactions between the solvent molecules and GO functional groups, the differences in the dielectric constants of water and ethanol, and the resulting changes in the charge state of GO sheets, which affect the interlayer electrostatic repulsion. The high polarity and strong hydrogen-bonding capacity of water enable GO to become highly hydrated and charged, thereby forming a stable dispersion. In contrast, the relatively hydrophobic nature and low dielectric constant of ethanol weaken the surface charge screening of GO, allowing van der Waals forces to dominate and leading to aggregation.40–42 The sheet-like graphene oxide, rich in surface oxygen groups, offers abundant anchoring sites for Mo precursors, thereby driving the nucleation and growth of MoS2 nanosheets on its surface.43,44 This intimate interfacial interaction produces dense MoS2 lattice fringes and yields MoGO-W with an interlayer spacing of only 0.86 nm—distinctly smaller than that of Solvo-MoS2 (0.93 nm ) and much smaller than that of MoGO-E (1.67 nm) (Fig. 3d, e and Fig. S3(a)). Water promotes uniform GO dispersion and stabilizes its morphology by forming strong hydrogen bonds and enhancing electrostatic repulsion, enabling dense vertical anchoring of monolayer MoS2 on GO sheets with abundant exposed edge sites, which in turn enhances catalytic activity.
![]() | ||
| Fig. 3 SEM pictures of (a) MoGO-W, (b) MoGO-E and (c) Solvo-MoS2. TEM pictures of the (d1–d3) MoGO-W and (e1–e3) MoGO-E catalysts. | ||
The microstructural morphology of the MoS2–GO catalysts with varying GO contents was characterized. For MoGO1 and MoGO1.5, the samples are composed of micron-sized spheres and sheets, with spheres being predominant (Fig. 4a and b). Upon magnification, the spherical particles and sheet surfaces are clearly visible, exhibiting a fuzzy texture. These correspond to the solvothermally synthesized MoS2 particles and MoS2–GO composite sheet clusters. As the GO doping amount increased, MoGO2 and MoGO2.5 were completely composed of micron-sized sheet clusters with fuzzy surfaces (Fig. 4c and d). This indicated that the Mo precursor can be fully anchored in the solvothermal environment, forming an expanded sheet structure with a high density of MoS2 distributed on the surface, by adjusting the GO content. However, excessive GO content in MoGO2.5 results in incomplete MoS2 coverage on the sheet surface, likely leading to insufficient active edge sites and reduced catalytic activity (Fig. 4d). Therefore, the appropriate ratio of Mo precursor to GO is crucial for achieving a uniform composite sheet cluster morphology. In the MoGO1 and MoGO1.5 catalysts, the MoS2 lattice fringes are mainly observed at the particle edges (Fig. S5). In contrast, in MoGO2 and MoGO2.5, the fringes are uniformly distributed across the GO surface, with a wider interlayer spacing observed. As the GO content increases, the MoS2 sheet length also significantly increases, from 3–4 nm in MoGO1 to 6–8 nm in MoGO2.5 (Fig. 3d and S5c). The interlayer spacing of the MoS2–GO catalysts was greater than the 0.62 nm of Solvo-MoS2, indicating an expanded monolayer structure.
![]() | ||
| Fig. 4 SEM pictures of the MoGO series catalysts with different GO contents (a1–a3: MoGO1, b1–b3: MoGO1.5, c1–c3: MoGO2, and d1–d3: MoGO2.5 ). | ||
All MoGO catalysts with varying GO contents exhibited Raman vibrational peaks characteristic of the 1T/MoS2 structure, indicating that they were monolayer structures (Fig. 5a). By comparing the peak intensity ratios of the D band and G band for each catalyst, it was found that the MoGO2 catalyst had the highest ID/IG ratio (MoGO1: 1.13, MoGO1.5: 1.33, MoGO2: 1.40, MoGO2.5: 1.32), reflecting its abundance of defect sites (Fig. 5b).37 Combining this with HRTEM characterization, it can be seen that as the GO content increases, the MoS2 sheet length in the MoS2–GO composite catalysts gradually increases, and the density of GO defect sites in the sheets improves. However, excessive aggregation of the sheets and poor expansiveness lead to a reduction in the number of GO defect sites.
![]() | ||
| Fig. 5 Raman spectra of MoGO series catalysts with different GO contents (a: 100–6000 cm−1, b: 1000–3000 cm−1). | ||
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| Fig. 6 HDS conversion and S(HYD/DDS) of DBT (a and c) and 4,6-DMDBT (b and d) catalyzed by the MoS2-based catalysts. | ||
We systematically evaluated the DBT HDS performance of MoGO catalysts bearing four different graphene oxide loadings. Under identical reaction conditions, DBT conversion and HYD selectivity exhibited a volcano-type trend as the GO loading increased. MoGO2 delivered the highest desulfurization activity (Fig. 6c). At temperatures below 280 °C, all four catalysts exhibited comparable HDS activity for 4,6-DMDBT. However, at higher temperatures, MoGO2's advantage became evident, achieving a 79.3% conversion at 300 °C (Fig. 6d). MoGO2 also exhibited superior HYD selectivity, with a HYD/DDS ratio of 12.8 for DBT HDS at 280 °C—significantly higher than those of the other catalysts (<10, Fig. 6c)—and a peak ratio of 14.8 for 4,6-DMDBT HDS at 320 °C (Fig. 6d). Kinetic analysis (Fig. S7) revealed that MoGO2 exhibited the lowest apparent activation energies—59.9 kJ mol−1 for DBT and 60.2 kJ mol−1 for 4,6-DMDBT—among the four catalysts, suggesting a larger Arrhenius pre-exponential factor and a higher density of active sites.48 These findings indicate that highly exfoliated graphene oxide sheets ensure uniform dispersion of MoS2, significantly enhancing active-site utilization and underpinning the exceptional HDS activity of MoGO2. Moreover, MoGO2 maintained high stability over 80 h of continuous operation, with DBT and 4,6-DMDBT conversions sustained at ∼90% and ∼79%, respectively, underscoring its exceptional catalytic durability and practical HDS potential (Fig. S8). In particular, the main product of the HDS of DBT is CBH, followed by BP.
The density of states (DOS) analysis for MoS2-1Layer, MoS2-2Layer, and MoS2–GO structures reveals that all three interfaces exhibit continuous energy band distributions near the Fermi level (EF), indicating good electron transfer capability (Fig. 7). Further examination of the projected density of states (PDOS) for Mo shows that the d-band center follows the order: MoS2-2Layer (−0.994 eV) < MoS2-1Layer (−0.799 eV) < MoS2–GO (−0.348 eV) (Fig. 7d). In the MoS2-2Layer structure, the strong interlayer interaction between the MoS2 layers causes electron transfer toward S atoms, shifting the d-band center further away from the Fermi level. In contrast, for the MoS2–GO structure, the d-band center is much closer to the Fermi level, indicating that the incorporation of GO enhances the electronic structure of Mo. Compared to MoS2-1Layer (4.940), the Bader charge of MoS2-2Layer (4.919) decreases, while that of MoS2–GO (4.965) increases, which is consistent with the d-band distribution results of PDOS (Table S4). This indicated that in the MoS2–GO composite structure obtained via the solvothermal method, GO influenced the electron density of monolayer MoS2, facilitating catalytic electron transfer.
![]() | ||
| Fig. 7 Density of states of (a) MoS2-1Layer, (b) MoS2-2Layer, and (c) MoS2–GO, and the projected DOS (d) of the above three structures. | ||
DFT calculations were conducted to investigate the adsorption and dissociation of H2 on three MoS2-based surfaces (Fig. 8a). The results showed that the adsorption energies of H2 on both MoS2-2Layer and MoS2–GO surfaces are similar, indicating chemisorption. Additionally, the dissociation energy of H2 was lower on both the MoS2-1Layer and MoS2–GO surfaces.
Given that the MoS2–GO catalysts exhibit higher selectivity for the HYD pathway, simulation calculations were performed to determine the energy barriers for DBT desulfurization via the hydrogenation pathway on the three MoS2 catalysts (Fig. 8b–d). In this pathway, DBT was initially hydrogenated to form tetrahydrodibenzothiophene (THDBT) (T1) and hexahydrodibenzothiophene (HHDBT) (T2). This was followed by desulfurization to yield CHB (T3), and further hydrogenation produces BCH (T4). The energy barriers for this reaction pathway were as follows: MoS2–GO (8.90 eV) < MoS2-1Layer (9.37 eV) < MoS2-2Layer (9.51 eV), confirming that MoS2–GO demonstrates the best catalytic performance for desulfurization through the HYD pathway.
Footnotes |
| † This paper is dedicated to Professor Zifeng Yan (School of Chemistry and Chemical Engineering, China University of Petroleum — East China) on the occasion of his 60th birthday. |
| ‡ Both of the authors contributed equally to this work. |
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