Xingju Zhao
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Xingju Zhao has a total of 76 co-authors. Here are the top co-authors by number of shared publications:
- Shunfang Li
Zhengzhou University
13 shared publications - Xiaoyan Ren
Key Laboratory of Material Physics, Ministry of Education, School of Physics, Zhengzhou University, Zhengzhou 450001, China
8 shared publications - Zhengxiao Guo
HKU‐CAS Joint Laboratory on New Materials & Department of Chemistry The University of Hong Kong Hong Kong SAR P. R. China
7 shared publications Xinlian Xue
Key Laboratory of Material Physics of Ministry of Education, School of Physics, Zhengzhou University, Zhengzhou, China
6 shared publicationsYandi Zhu
Zhengzhou University
6 shared publicationsJinlei Shi
College of physics and Electronic Engineering, Zhengzhou Normal University, Zhengzhou 450044, China
5 shared publications
Latest Publications
- 24 August 2026
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 10 (8) , 086001
Prediction of the lightest three-dimensional diamond-like fullerene phase with orbital-coupling-tunable pseudo-Dirac states and flat band states
The discovery of novel carbon allotropes---from fullerenes and nanotubes to graphene---has greatly advanced contemporary materials research. Beyond conventional atomic crystals, superatomic solids provide an attractive platform for exploring structure-property relationships arising from their unique hierarchical architectures. Here, using state-of-the-art first-principles calculations, we propose a three-dimensional (3D) diamond-like fullerene (${\mathrm{C}}_{60}$) phase, dubbed fullerdiamond (FLD), constructed by substituting each carbon atom in diamond with a ${\mathrm{C}}_{60}$ superatom, where each ${\mathrm{C}}_{60}$ covalently connects to its four neighbors via four 66/66 [2+2] cycloadditions. Our calculations reveal that FLD is structurally stable, with the lowest density (1.098 $\mathrm{g}/{\mathrm{cm}}^{3}$) among diamond-type structures and anisotropic Young's moduli of $50.91\ensuremath{\sim}85.35$ GPa. Its electronic structure exhibits a sizable indirect band gap of 1.83 eV and two distinctive features: (i) an accidental pseudo-Dirac cone (\ensuremath{\sim}57 meV gap) in the conduction band arising from antibonding coupling between LUMO states of neighboring ${\mathrm{C}}_{60}$ superatoms, and (ii) a narrow flat band (\ensuremath{\sim}104 meV) in the valence band. Moreover, a tensile strain of \ensuremath{\sim}3% along the [100] direction weakens the antibonding orbital coupling between neighboring ${\mathrm{C}}_{60}$ superatoms through elongation of the inter-cage [2+2] cycloaddition bonds, reducing the accidental pseudo-Dirac gap to \ensuremath{\sim}4 meV and narrowing the flat band width to \ensuremath{\sim}88 meV. This strain-tunable electronic behavior---arising from the sensitivity of inter-${\mathrm{C}}_{60}$ orbital coupling to lattice deformation---establishes a conceptual bridge between fullerene molecular physics and diamond-like 3D superatomic solid physics. Our findings highlight FLD as a promising platform for tuning electronic and optical properties in lightweight carbon-based materials.- 24 August 2026
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 10 (8) , 086001
Prediction of the lightest three-dimensional diamond-like fullerene phase with orbital-coupling-tunable pseudo-Dirac states and flat band states
The discovery of novel carbon allotropes---from fullerenes and nanotubes to graphene---has greatly advanced contemporary materials research. Beyond conventional atomic crystals, superatomic solids provide an attractive platform for exploring structure-property relationships arising from their unique hierarchical architectures. Here, using state-of-the-art first-principles calculations, we propose a three-dimensional (3D) diamond-like fullerene (${\mathrm{C}}_{60}$) phase, dubbed fullerdiamond (FLD), constructed by substituting each carbon atom in diamond with a ${\mathrm{C}}_{60}$ superatom, where each ${\mathrm{C}}_{60}$ covalently connects to its four neighbors via four 66/66 [2+2] cycloadditions. Our calculations reveal that FLD is structurally stable, with the lowest density (1.098 $\mathrm{g}/{\mathrm{cm}}^{3}$) among diamond-type structures and anisotropic Young's moduli of $50.91\ensuremath{\sim}85.35$ GPa. Its electronic structure exhibits a sizable indirect band gap of 1.83 eV and two distinctive features: (i) an accidental pseudo-Dirac cone (\ensuremath{\sim}57 meV gap) in the conduction band arising from antibonding coupling between LUMO states of neighboring ${\mathrm{C}}_{60}$ superatoms, and (ii) a narrow flat band (\ensuremath{\sim}104 meV) in the valence band. Moreover, a tensile strain of \ensuremath{\sim}3% along the [100] direction weakens the antibonding orbital coupling between neighboring ${\mathrm{C}}_{60}$ superatoms through elongation of the inter-cage [2+2] cycloaddition bonds, reducing the accidental pseudo-Dirac gap to \ensuremath{\sim}4 meV and narrowing the flat band width to \ensuremath{\sim}88 meV. This strain-tunable electronic behavior---arising from the sensitivity of inter-${\mathrm{C}}_{60}$ orbital coupling to lattice deformation---establishes a conceptual bridge between fullerene molecular physics and diamond-like 3D superatomic solid physics. Our findings highlight FLD as a promising platform for tuning electronic and optical properties in lightweight carbon-based materials.- 2 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (11)
Quantifying humidity effects on commensurability-dependent friction in bilayer graphene: A generalized registry index model
- 2 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (11)
Quantifying humidity effects on commensurability-dependent friction in bilayer graphene: A generalized registry index model
- 8 September 2025
- Published by Springer Nature in Science China Physics, Mechanics & Astronomy
- Vol. 68 (12) , 1-9
Fullerphene: A double covalently bonded two-dimensional fullerene semiconducting crystal with preserved Dirac states and emergent flat bands
- 8 September 2025
- Published by Springer Nature in Science China Physics, Mechanics & Astronomy
- Vol. 68 (12) , 1-9
Fullerphene: A double covalently bonded two-dimensional fullerene semiconducting crystal with preserved Dirac states and emergent flat bands
- 4 October 2024
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry A
- Vol. 12 (44) , 30498-30507
Catalytic kinetic growth of a half-metallic hexagonal boron nitride-graphene lateral heterostructure using transition metal single-atom catalysts on Rh(111)
Deciphering the precise catalytic growth mechanism of atomically thin graphene-based lateral heterostructures is of great interest in low-dimensional physics and materials. Here, based on first-principles calculations and extensive screenings, we reveal that the deposited transition metal atoms (TM = Mn, Zr, Nb, Mo, Hf, Ta, and W), particularly Mo, act as single-atom catalysts (SACs) to effectively promote C adatom dimerization both energetically and kinetically on a C-dimer-unpreferred Rh(111) substrate. Meanwhile, the TM-SAC increases the stability of the boron-nitride (BN) dimer, which promotes rapid growth of a hexagonal boron nitride-graphene (h-BN-G) lateral heterostructure. Specifically, taking TM = Mo as a typical example, we demonstrate that the Mo–C(BN) couplings weaken the C(BN)-substrate interactions, which sharply reduces the kinetic barriers for both C and BN nucleation and migration in the initial stage of growing the h-BN-G lateral heterostructure on Rh(111). Interestingly, Mo-SAC can dynamically involve and migrate out of the h-BN-G interface during the growth processes for C2 dimers as feeding blocks. Moreover, the presence of Mo-SAC can effectively tune the patching boundary of the 1D h-BN-G heterostructure, i.e., from C–N to C–B linking with half-metallicity. The present findings provide significantly new insights into controllable catalytic growth of two-dimensional (2D) lateral heterostructures with various important potential applications, such as transport in spintronic devices.
- 4 October 2024
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry A
- Vol. 12 (44) , 30498-30507
Catalytic kinetic growth of a half-metallic hexagonal boron nitride-graphene lateral heterostructure using transition metal single-atom catalysts on Rh(111)
Deciphering the precise catalytic growth mechanism of atomically thin graphene-based lateral heterostructures is of great interest in low-dimensional physics and materials. Here, based on first-principles calculations and extensive screenings, we reveal that the deposited transition metal atoms (TM = Mn, Zr, Nb, Mo, Hf, Ta, and W), particularly Mo, act as single-atom catalysts (SACs) to effectively promote C adatom dimerization both energetically and kinetically on a C-dimer-unpreferred Rh(111) substrate. Meanwhile, the TM-SAC increases the stability of the boron-nitride (BN) dimer, which promotes rapid growth of a hexagonal boron nitride-graphene (h-BN-G) lateral heterostructure. Specifically, taking TM = Mo as a typical example, we demonstrate that the Mo–C(BN) couplings weaken the C(BN)-substrate interactions, which sharply reduces the kinetic barriers for both C and BN nucleation and migration in the initial stage of growing the h-BN-G lateral heterostructure on Rh(111). Interestingly, Mo-SAC can dynamically involve and migrate out of the h-BN-G interface during the growth processes for C2 dimers as feeding blocks. Moreover, the presence of Mo-SAC can effectively tune the patching boundary of the 1D h-BN-G heterostructure, i.e., from C–N to C–B linking with half-metallicity. The present findings provide significantly new insights into controllable catalytic growth of two-dimensional (2D) lateral heterostructures with various important potential applications, such as transport in spintronic devices.
- 5 September 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (12) , 125405
Covalent-bond-linked monolayer fullerene network as a spin sponge for spin-triplet activation and CO oxidationRecently, a novel class of 2D carbon material, covalent-bond-linked monolayer networks with quasihexagonal phase (qHP-) was experimentally fabricated [Hou et al., Nature (London) 606, 507 (2022)]. Here, using first-principles calculations, we predict that such a two-dimensional network serves as an ideal platform in stabilizing transition metals (TM: Mn, Fe, Co, and Ni) into dispersive single atoms, exhibiting remarkable efficiency for spin-triplet activation and CO oxidation with low reaction barriers . First, the two-dimensional qHP- network acts as an electronic reservoir responsible for charge transfer to the antibonding orbital of . Second, and important, it functions as a spin sponge in accommodation of the reduced spin magnetic moment from molecule, facilitating its spin triplet-to-singlet transition in the framework of Wigner's spin conservation rule. Delicate quantitative calculations demonstrate that the spin component contributes approximately twice as significantly as that of pure charge transfer in reducing the activation barrier for CO oxidation.- 5 September 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (12) , 125405
Covalent-bond-linked monolayer fullerene network as a spin sponge for spin-triplet activation and CO oxidationRecently, a novel class of 2D carbon material, covalent-bond-linked monolayer networks with quasihexagonal phase (qHP-) was experimentally fabricated [Hou et al., Nature (London) 606, 507 (2022)]. Here, using first-principles calculations, we predict that such a two-dimensional network serves as an ideal platform in stabilizing transition metals (TM: Mn, Fe, Co, and Ni) into dispersive single atoms, exhibiting remarkable efficiency for spin-triplet activation and CO oxidation with low reaction barriers . First, the two-dimensional qHP- network acts as an electronic reservoir responsible for charge transfer to the antibonding orbital of . Second, and important, it functions as a spin sponge in accommodation of the reduced spin magnetic moment from molecule, facilitating its spin triplet-to-singlet transition in the framework of Wigner's spin conservation rule. Delicate quantitative calculations demonstrate that the spin component contributes approximately twice as significantly as that of pure charge transfer in reducing the activation barrier for CO oxidation.- 19 August 2024
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry A
- Vol. 128 (41) , 8856-8864
Energetic and Kinetic Competition on the Stability of Pd13 Clusters: Ab Initio Molecular Dynamics Simulations
Material stability is the focus on both experiments and calculations, which includes the energetic stability at the static state and the thermodynamic stability at the kinetic state. To show whether energetics or kinetics dominates on material stability, this study focuses on the Pd-13 clusters, because of their observable magnetic moment in experiment. Energetically, the CALYPSO searching method and first-principles calculations find that Pd-13(C-2) is the ground state at 0 K while the static frequency calculations demonstrate that the icosahedron Pd-13(I-h) becomes more favorable on free energy as temperature increases. However, their magnetic moments (8 mu(B)) are not in agreement with the experimental value (<5.2 mu(B)). Kinetically, ab initio molecular dynamics simulations reveal that Pd-13(C-3v) (6 mu(B)) has supreme isomerization temperature and the other 11 low-lying isomers transform to Pd-13(C-3v) directly or indirectly, demonstrating that Pd-13(C-3v) has the maximum probability to be observed in experiment. The magnetic moment difference between experiment (<5.2 mu(B)) and this calculation (6 mu(B)) may be due to the spin multiplicities. Our result suggests that the magnetic moment disparity between theory and experiment (in Pd-13 clusters) originates from the kinetic stability.
- 19 August 2024
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry A
- Vol. 128 (41) , 8856-8864
Energetic and Kinetic Competition on the Stability of Pd13 Clusters: Ab Initio Molecular Dynamics Simulations
Material stability is the focus on both experiments and calculations, which includes the energetic stability at the static state and the thermodynamic stability at the kinetic state. To show whether energetics or kinetics dominates on material stability, this study focuses on the Pd-13 clusters, because of their observable magnetic moment in experiment. Energetically, the CALYPSO searching method and first-principles calculations find that Pd-13(C-2) is the ground state at 0 K while the static frequency calculations demonstrate that the icosahedron Pd-13(I-h) becomes more favorable on free energy as temperature increases. However, their magnetic moments (8 mu(B)) are not in agreement with the experimental value (<5.2 mu(B)). Kinetically, ab initio molecular dynamics simulations reveal that Pd-13(C-3v) (6 mu(B)) has supreme isomerization temperature and the other 11 low-lying isomers transform to Pd-13(C-3v) directly or indirectly, demonstrating that Pd-13(C-3v) has the maximum probability to be observed in experiment. The magnetic moment difference between experiment (<5.2 mu(B)) and this calculation (6 mu(B)) may be due to the spin multiplicities. Our result suggests that the magnetic moment disparity between theory and experiment (in Pd-13 clusters) originates from the kinetic stability.
- 25 May 2024
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 26 (23) , 16459-16465
Spin-polarized p-block antimony/bismuth single-atom catalysts on defect-free rutile TiO2(110) substrate for highly efficient CO oxidation
We establish a new strategy for constructing spin-polarized single Bi/Sb atoms on defect-free TiO2(110), showing excellent catalytic activities for spin-triplet O2 activation and CO oxidation with low rate-limiting reaction barrier of ∼0.6 eV.
- 25 May 2024
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 26 (23) , 16459-16465
Spin-polarized p-block antimony/bismuth single-atom catalysts on defect-free rutile TiO2(110) substrate for highly efficient CO oxidation
We establish a new strategy for constructing spin-polarized single Bi/Sb atoms on defect-free TiO2(110), showing excellent catalytic activities for spin-triplet O2 activation and CO oxidation with low rate-limiting reaction barrier of ∼0.6 eV.
- Open Access
- 20 February 2024
- Published by National Academy of Sciences in Proceedings of the National Academy of Sciences
- Vol. 121 (9)
Centimeter-sized diamond composites with high electrical conductivity and hardness
Achieving high-performance materials with superior mechanical properties and electrical conductivity, especially in large-sized bulk forms, has always been the goal. However, it remains a grand challenge due to the inherent trade-off between these properties. Herein, by employing nanodiamonds as precursors, centimeter-sized diamond/graphene composites were synthesized under moderate pressure and temperature conditions (12 GPa and 1,300 to 1,500 °C), and the composites consisted of ultrafine diamond grains and few-layer graphene domains interconnected through covalently bonded interfaces. The composites exhibit a remarkable electrical conductivity of 2.0 × 10 4 S m −1 at room temperature, a Vickers hardness of up to ~55.8 GPa, and a toughness of 10.8 to 19.8 MPa m 1/2 . Theoretical calculations indicate that the transformation energy barrier for the graphitization of diamond surface is lower than that for diamond growth directly from conventional sp 2 carbon materials, allowing the synthesis of such diamond composites under mild conditions. The above results pave the way for realizing large-sized diamond-based materials with ultrahigh electrical conductivity and superior mechanical properties simultaneously under moderate synthesis conditions, which will facilitate their large-scale applications in a variety of fields.
- 20 February 2024
- Published by National Academy of Sciences in Proceedings of the National Academy of Sciences
- Vol. 121 (9)
Open AccessCentimeter-sized diamond composites with high electrical conductivity and hardness
Achieving high-performance materials with superior mechanical properties and electrical conductivity, especially in large-sized bulk forms, has always been the goal. However, it remains a grand challenge due to the inherent trade-off between these properties. Herein, by employing nanodiamonds as precursors, centimeter-sized diamond/graphene composites were synthesized under moderate pressure and temperature conditions (12 GPa and 1,300 to 1,500 °C), and the composites consisted of ultrafine diamond grains and few-layer graphene domains interconnected through covalently bonded interfaces. The composites exhibit a remarkable electrical conductivity of 2.0 × 10 4 S m −1 at room temperature, a Vickers hardness of up to ~55.8 GPa, and a toughness of 10.8 to 19.8 MPa m 1/2 . Theoretical calculations indicate that the transformation energy barrier for the graphitization of diamond surface is lower than that for diamond growth directly from conventional sp 2 carbon materials, allowing the synthesis of such diamond composites under mild conditions. The above results pave the way for realizing large-sized diamond-based materials with ultrahigh electrical conductivity and superior mechanical properties simultaneously under moderate synthesis conditions, which will facilitate their large-scale applications in a variety of fields.
- 20 February 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 109 (8) , 085420
Negative differential friction predicted in two-dimensional electride commensurate contacts: Role of the electronic structure
In recent decade, structural superlubricity has been established as one of the most effective methods to achieve extremely low friction when two crystalline surfaces slide over each other in dry incommensurate contact, which however may be blocked to commensurate configurations during the sliding and thus lead the failure of superlubricity. Here, our first-principles calculations predict negative differential static friction coefficient in the commensurate contact of bilayer two-dimensional (2D) electride (such as , , and ), which was essentially sustained by the concept of electronic lubricity, where the lubricity was dominated by the electronic structures, rather than the structural effect. Specifically, it is demonstrated that, in the range of 0–10 GPa, the pressure-enhanced charge transfer from the vicinity of surface Ca and interfacial Ca atoms to the uniformly distributed interstitial anionic electron regime collectively screens the corrugation of the sliding potential energy surface (PES) and thus leads to negative differential friction coefficient μ. However, beyond 10 GPa, the accumulated interstitial anionic electrons become significantly localized when sliding to the saddle point of the PES, thus leading to much enhanced electronic kinetic energy, leading to positive μ. The present findings on electronic lubricity are expected to play an instrumental role in developing high-performance solid lubricants.- 20 February 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 109 (8) , 085420
Negative differential friction predicted in two-dimensional electride commensurate contacts: Role of the electronic structure
In recent decade, structural superlubricity has been established as one of the most effective methods to achieve extremely low friction when two crystalline surfaces slide over each other in dry incommensurate contact, which however may be blocked to commensurate configurations during the sliding and thus lead the failure of superlubricity. Here, our first-principles calculations predict negative differential static friction coefficient in the commensurate contact of bilayer two-dimensional (2D) electride (such as , , and ), which was essentially sustained by the concept of electronic lubricity, where the lubricity was dominated by the electronic structures, rather than the structural effect. Specifically, it is demonstrated that, in the range of 0–10 GPa, the pressure-enhanced charge transfer from the vicinity of surface Ca and interfacial Ca atoms to the uniformly distributed interstitial anionic electron regime collectively screens the corrugation of the sliding potential energy surface (PES) and thus leads to negative differential friction coefficient μ. However, beyond 10 GPa, the accumulated interstitial anionic electrons become significantly localized when sliding to the saddle point of the PES, thus leading to much enhanced electronic kinetic energy, leading to positive μ. The present findings on electronic lubricity are expected to play an instrumental role in developing high-performance solid lubricants.- 9 August 2023
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry A
- Vol. 11 (35) , 19138-19144
Hydrogen-assisted growth of single crystalline borophene investigated by first-principles calculations
The development of an effective method for mass production of single crystalline two-dimensional (2D) materials is still a standing challenge. Here, using first-principles calculations, we predict the crucial role of the simplest and the most abundant element in the universe, hydrogen, as a surfactant in mass production of single crystalline borophene grown on Ag(111). Specifically, hydrogen not only readily induces the dissolved B atoms to segregate onto the Ag(111) substrate, but also promotes the B atoms to fast nucleate via changing the repulsive pairwise interactions of B atoms to be attractive. Importantly, the introduction of a small amount of hydrogen saturation on the edges (the H/B ratio is lower than 1 : 6) effectively lifts the degeneracy of the baby-islands between two most stable borophene phases that are experimentally fabricated, effectively promoting single crystalline growth, via distinct minimization of their edge energies as rationalized by the generalized Wulff construction. The present findings may open a new avenue toward mass production of borophene and other single crystalline 2D materials, and the hydrogen passivation on the edges may facilitate the exfoliation of borophene grown on metal substrates and thus promote the subsequent characterization or applications.
- 9 August 2023
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry A
- Vol. 11 (35) , 19138-19144
Hydrogen-assisted growth of single crystalline borophene investigated by first-principles calculations
The development of an effective method for mass production of single crystalline two-dimensional (2D) materials is still a standing challenge. Here, using first-principles calculations, we predict the crucial role of the simplest and the most abundant element in the universe, hydrogen, as a surfactant in mass production of single crystalline borophene grown on Ag(111). Specifically, hydrogen not only readily induces the dissolved B atoms to segregate onto the Ag(111) substrate, but also promotes the B atoms to fast nucleate via changing the repulsive pairwise interactions of B atoms to be attractive. Importantly, the introduction of a small amount of hydrogen saturation on the edges (the H/B ratio is lower than 1 : 6) effectively lifts the degeneracy of the baby-islands between two most stable borophene phases that are experimentally fabricated, effectively promoting single crystalline growth, via distinct minimization of their edge energies as rationalized by the generalized Wulff construction. The present findings may open a new avenue toward mass production of borophene and other single crystalline 2D materials, and the hydrogen passivation on the edges may facilitate the exfoliation of borophene grown on metal substrates and thus promote the subsequent characterization or applications.