Bin Wen
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
Bin Wen has a total of 282 co-authors. Here are the top co-authors by number of shared publications:
- Changzeng Fan
State Key Laboratory of Metastable Materials Science and Technology, Yanshan University, Qinhuangdao 066004, People's Republic of China
26 shared publications - Lifeng Zhang
North China University of Technology
18 shared publications - Roderick Melnik
Wilfrid Laurier University
18 shared publications Xing Feng
12 shared publicationsYoshiyuki Kawazoe
New Industry Creation Hatchery Center, Tohoku University, 6-6-4 Aramaki-aza-Aoba, Aoba-ku, Sendai, 980-8579, Japan
10 shared publications- Yibo Liu
State Key Laboratory of Metastable Materials Science and Technology, Yanshan University, Qinhuangdao 066004, People's Republic of China
9 shared publications
Latest Publications
- Open Access
- 22 October 2026
- Published by Wiley in Advanced Functional Materials
- p. e79033
Sacrificing Initial Active Area for Superior Structural and Interfacial Stability in MoSe 2 /C Anodes for All‐Solid‐State Lithium Batteries
Conversion‐type materials for all‐solid‐state lithium batteries face low conductivity, sluggish kinetics, severe volume expansion, and unstable interfaces. Herein, a MoSe 2 /C composite is fabricated via a wet‐chemical synthesis approach combined with shell engineering. Density functional theory calculations show that the carbon skeleton enhances conductivity, improves Li + adsorption, and lowers the diffusion barrier. In situ and finite element analyses confirm that the hollow carbon mitigates volume expansion and redistributes stress. Distribution of relaxation times analysis reveals that stress buffering suppresses interfacial degradation and enhances Li + migration. Pseudocapacitive analysis shows a slightly higher contribution for pristine MoSe 2 due to face‐to‐face stacking versus point‐contact packing in MoSe 2 /C, which sacrifices some initial active area. However, the carbon skeleton accelerates the kinetics of the remaining active regions and provides excellent stress buffering and interfacial stability. Consequently, the MoSe 2 /C anode exhibits rate capability and long‐term cycling performance in both half‐cells (11 000 cycles at 3 A g −1 ) and full‐cells (200 cycles at 0.1 C). This work proposes a counterintuitive strategy of “trading part of the initial active area in exchange for superior structural and interfacial stability,” offering a rational design paradigm for conversion‐type materials.
- 22 October 2026
- Published by Wiley in Advanced Functional Materials
- p. e79033
Open AccessSacrificing Initial Active Area for Superior Structural and Interfacial Stability in MoSe 2 /C Anodes for All‐Solid‐State Lithium Batteries
Conversion‐type materials for all‐solid‐state lithium batteries face low conductivity, sluggish kinetics, severe volume expansion, and unstable interfaces. Herein, a MoSe 2 /C composite is fabricated via a wet‐chemical synthesis approach combined with shell engineering. Density functional theory calculations show that the carbon skeleton enhances conductivity, improves Li + adsorption, and lowers the diffusion barrier. In situ and finite element analyses confirm that the hollow carbon mitigates volume expansion and redistributes stress. Distribution of relaxation times analysis reveals that stress buffering suppresses interfacial degradation and enhances Li + migration. Pseudocapacitive analysis shows a slightly higher contribution for pristine MoSe 2 due to face‐to‐face stacking versus point‐contact packing in MoSe 2 /C, which sacrifices some initial active area. However, the carbon skeleton accelerates the kinetics of the remaining active regions and provides excellent stress buffering and interfacial stability. Consequently, the MoSe 2 /C anode exhibits rate capability and long‐term cycling performance in both half‐cells (11 000 cycles at 3 A g −1 ) and full‐cells (200 cycles at 0.1 C). This work proposes a counterintuitive strategy of “trading part of the initial active area in exchange for superior structural and interfacial stability,” offering a rational design paradigm for conversion‐type materials.
- 21 July 2026
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 165 (3)
GTAttn-XC: Physically constrained attention for nonlocal density functionals.
Machine-learning-based nonlocal density functional approximations have demonstrated substantial potential in advancing the applicability of electronic density functional theory. However, most existing approaches rely on handcrafted local or nonlocal descriptors, which limits their scalability in modeling long-range electronic responses. In this work, we propose a novel exchange-correlation functional approximation model-GTAttn-XC, which introduces a learnable attention mechanism to enable unsupervised modeling of long-range electronic responses. By coupling a multiscale real-space grid graph representation with attention operators, the proposed method achieves a unified description of local accuracy and nonlocal interactions, while avoiding the computational overhead associated with explicit high-order correlation terms. Evaluations on multiple benchmark datasets, including MGCDB84, demonstrate that the model consistently delivers high accuracy across a range of tasks, such as weak interactions, reaction energies, barrier heights, and thermochemical energies. These results establish a new technical pathway toward high-accuracy nonlocal exchange-correlation approximations.
- 21 July 2026
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 165 (3)
GTAttn-XC: Physically constrained attention for nonlocal density functionals.
Machine-learning-based nonlocal density functional approximations have demonstrated substantial potential in advancing the applicability of electronic density functional theory. However, most existing approaches rely on handcrafted local or nonlocal descriptors, which limits their scalability in modeling long-range electronic responses. In this work, we propose a novel exchange-correlation functional approximation model-GTAttn-XC, which introduces a learnable attention mechanism to enable unsupervised modeling of long-range electronic responses. By coupling a multiscale real-space grid graph representation with attention operators, the proposed method achieves a unified description of local accuracy and nonlocal interactions, while avoiding the computational overhead associated with explicit high-order correlation terms. Evaluations on multiple benchmark datasets, including MGCDB84, demonstrate that the model consistently delivers high accuracy across a range of tasks, such as weak interactions, reaction energies, barrier heights, and thermochemical energies. These results establish a new technical pathway toward high-accuracy nonlocal exchange-correlation approximations.
- 1 July 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (1)
Computational method to predict yield strength under static high pressure: Al and Ag as prototypes
- 1 July 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (1)
Computational method to predict yield strength under static high pressure: Al and Ag as prototypes
- Open Access
- 22 June 2026
- Published by Springer Nature in Nature Communications
- Vol. 17 (1)
Anion-exchange fluorinated ion conductors for stable high-voltage lithium battery
The development of high-energy all-solid-state batteries is critically hindered by the electrochemical instability of solid electrolytes against high-voltage oxide positive electrodes. While fluorination is a promising strategy to enhance electrolyte stability, conventional methods are ineffective, resulting in insufficient fluorine content and a debilitating trade-off with ionic conductivity. Here, we report a solid-state anion-exchange strategy that overcomes these limitations by producing core-shell Li-fluoride/LiCl nanocomposite precursors. These precursors enable the synthesis of heavily fluorinated lithium-halide and lithium-sulfide electrolytes that combine high ionic conductivity with good oxidative stability. This stability originates from the formation of a robust, self-limiting LiF-rich interphase at the positive electrode. Consequently, an all-solid-state battery using a Li-rich oxide positive electrode achieves high performance, retaining over 77.5% capacity after 2000 cycles at a high rate of 3 C (1 C = 275 mA/g) and a 5.0 V cutoff. This anion-exchange approach is broadly applicable to other systems and establishes a versatile platform for designing advanced fluorinated materials for next-generation batteries.
- 22 June 2026
- Published by Springer Nature in Nature Communications
- Vol. 17 (1)
Open AccessAnion-exchange fluorinated ion conductors for stable high-voltage lithium battery
The development of high-energy all-solid-state batteries is critically hindered by the electrochemical instability of solid electrolytes against high-voltage oxide positive electrodes. While fluorination is a promising strategy to enhance electrolyte stability, conventional methods are ineffective, resulting in insufficient fluorine content and a debilitating trade-off with ionic conductivity. Here, we report a solid-state anion-exchange strategy that overcomes these limitations by producing core-shell Li-fluoride/LiCl nanocomposite precursors. These precursors enable the synthesis of heavily fluorinated lithium-halide and lithium-sulfide electrolytes that combine high ionic conductivity with good oxidative stability. This stability originates from the formation of a robust, self-limiting LiF-rich interphase at the positive electrode. Consequently, an all-solid-state battery using a Li-rich oxide positive electrode achieves high performance, retaining over 77.5% capacity after 2000 cycles at a high rate of 3 C (1 C = 275 mA/g) and a 5.0 V cutoff. This anion-exchange approach is broadly applicable to other systems and establishes a versatile platform for designing advanced fluorinated materials for next-generation batteries.
- 29 May 2026
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 65 (23) , 12886-12894
Discovery of Mg 3 Zn 2 Intermetallic Phase in the Mg–Zn System Enabled by Neuroevolution Potentials
Magnesium–zinc (Mg–Zn) alloys derive much of their mechanical strength from the formation and evolution of intermetallic compounds. However, the Mg-rich and intermediate compositional regimes remain insufficiently resolved structurally, hindering a comprehensive and phase-consistent understanding of phase stability and its role in microstructural strengthening. Here, we develop a high-accuracy neuroevolution potential (NEP) for the Mg–Zn system by integrating an active-learning strategy with the CALYPSO structure-search method, enabling systematic exploration of complex configurational phase space with near-first-principles accuracy. Extensive NEP-assisted structure searches reproduce all experimentally established Mg–Zn intermetallic phases and predict a previously unreported thermodynamically stable Mg3Zn2 phase with P42/mnm symmetry, together with a metastable I4/mcm-Mg2Zn phase. Mg3Zn2 is a plausible candidate constituent phase, as a selected simulated X-ray diffraction feature is consistent with an unassigned peak previously reported in multiphase Mg–Zn alloys. Additionally, Mg3Zn2 exhibits superior thermal robustness, retaining higher strength and hardness at elevated temperatures compared with the widely studied MgZn2. These results demonstrate the effectiveness of NEP-assisted structure prediction in resolving hidden intermetallic phases and establishing systematic structure–property relationships in chemically complex alloy systems.
- 29 May 2026
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 65 (23) , 12886-12894
Discovery of Mg 3 Zn 2 Intermetallic Phase in the Mg–Zn System Enabled by Neuroevolution Potentials
Magnesium–zinc (Mg–Zn) alloys derive much of their mechanical strength from the formation and evolution of intermetallic compounds. However, the Mg-rich and intermediate compositional regimes remain insufficiently resolved structurally, hindering a comprehensive and phase-consistent understanding of phase stability and its role in microstructural strengthening. Here, we develop a high-accuracy neuroevolution potential (NEP) for the Mg–Zn system by integrating an active-learning strategy with the CALYPSO structure-search method, enabling systematic exploration of complex configurational phase space with near-first-principles accuracy. Extensive NEP-assisted structure searches reproduce all experimentally established Mg–Zn intermetallic phases and predict a previously unreported thermodynamically stable Mg3Zn2 phase with P42/mnm symmetry, together with a metastable I4/mcm-Mg2Zn phase. Mg3Zn2 is a plausible candidate constituent phase, as a selected simulated X-ray diffraction feature is consistent with an unassigned peak previously reported in multiphase Mg–Zn alloys. Additionally, Mg3Zn2 exhibits superior thermal robustness, retaining higher strength and hardness at elevated temperatures compared with the widely studied MgZn2. These results demonstrate the effectiveness of NEP-assisted structure prediction in resolving hidden intermetallic phases and establishing systematic structure–property relationships in chemically complex alloy systems.
- Open Access
- 19 March 2026
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 11 (3) , x260266
Crystal structure of Al 8.77 Fe 0.80 Ni 1.20 Si 0.23
The Al 8.77 Fe 0.80 Ni 1.20 Si 0.23 (aluminium iron nickel silicate) phase, obtained via high-pressure sintering of an Al-rich prealloy (nominal composition Al 78.08 Fe 8.65 Ni 8.69 Si 4.58 ), is characterized as a novel phase in the Al—Si—Ni—Fe quaternary system. The obtained phase crystallizes in the space group P 2 1 / c , with lattice parameters a = 6.2093 (9), b = 6.2579 (9), c = 8.5661 (12) Å, and β = 94.877 (5)°. It is isotypic with Al 9 Fe 0.7 Ni 1.28 [ a = 6.2406 (1), b = 6.2993 (1), c = 8.5992 (1) Å, and β = 95.129 (1)°; Chumak et al. (2007). Intermetallics , 15 , 1416–1424] and Co 2 Al 9 [ a = 6.2163 (3), b = 6.2883 (3), c = 8.5587 (3) Å, and β = 94.772 (4)°; Boström et al. (2005). Z. Anorg. Allg. Chem . 631 , 534–541]. It features a co-occupancy of Al and Si atoms with a ratio of the refined site-occupancy factors of 0.88 (10):0.12 (10), as well a co-occupancy Ni/Fe with site-occupancy factors of 0.60 (4):0.40 (4).
- 19 March 2026
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 11 (3) , x260266
Open AccessCrystal structure of Al 8.77 Fe 0.80 Ni 1.20 Si 0.23
The Al 8.77 Fe 0.80 Ni 1.20 Si 0.23 (aluminium iron nickel silicate) phase, obtained via high-pressure sintering of an Al-rich prealloy (nominal composition Al 78.08 Fe 8.65 Ni 8.69 Si 4.58 ), is characterized as a novel phase in the Al—Si—Ni—Fe quaternary system. The obtained phase crystallizes in the space group P 2 1 / c , with lattice parameters a = 6.2093 (9), b = 6.2579 (9), c = 8.5661 (12) Å, and β = 94.877 (5)°. It is isotypic with Al 9 Fe 0.7 Ni 1.28 [ a = 6.2406 (1), b = 6.2993 (1), c = 8.5992 (1) Å, and β = 95.129 (1)°; Chumak et al. (2007). Intermetallics , 15 , 1416–1424] and Co 2 Al 9 [ a = 6.2163 (3), b = 6.2883 (3), c = 8.5587 (3) Å, and β = 94.772 (4)°; Boström et al. (2005). Z. Anorg. Allg. Chem . 631 , 534–541]. It features a co-occupancy of Al and Si atoms with a ratio of the refined site-occupancy factors of 0.88 (10):0.12 (10), as well a co-occupancy Ni/Fe with site-occupancy factors of 0.60 (4):0.40 (4).
- Open Access
- 21 November 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (11)
Al 48.18 Cr 22.78 Fe 4.04 Si 3
A mixture with the initial chemical composition Al 59 Cr 21 Fe 10 Si 10 was subjected to high-pressure sintering, resulting in the unexpected synthesis of an intermetallic compound with the composition Al 48.18 Cr 22.78 Fe 4.04 Si 3 , which adopts the Cr 0.88 Fe 0.12 Ga structure type in the space group R 3 m . Structural analysis indicates that Al, Cr and Fe jointly occupy a special position (Wyckoff site 18 h ), with refined site occupancy factors of 0.676 (6), 0.17 (2) and 0.16 (2), respectively. Cr and Fe share another special position (Wyckoff site 3 b ), with refined site occupancy factors of 0.60 (6) and 0.40 (6), respectively. Other atoms in the crystal (Al and Si) fully occupy their sites.
- 21 November 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (11)
Open AccessAl 48.18 Cr 22.78 Fe 4.04 Si 3
A mixture with the initial chemical composition Al 59 Cr 21 Fe 10 Si 10 was subjected to high-pressure sintering, resulting in the unexpected synthesis of an intermetallic compound with the composition Al 48.18 Cr 22.78 Fe 4.04 Si 3 , which adopts the Cr 0.88 Fe 0.12 Ga structure type in the space group R 3 m . Structural analysis indicates that Al, Cr and Fe jointly occupy a special position (Wyckoff site 18 h ), with refined site occupancy factors of 0.676 (6), 0.17 (2) and 0.16 (2), respectively. Cr and Fe share another special position (Wyckoff site 3 b ), with refined site occupancy factors of 0.60 (6) and 0.40 (6), respectively. Other atoms in the crystal (Al and Si) fully occupy their sites.
- Open Access
- 21 November 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (11)
(Al 13.28 Si 2.72 )(Fe 1.19 Ni 2.81 )
The intermetallic phase (Al 13.28 Si 2.72 )(Fe 1.19 Ni 2.81 ) was obtained by high-pressure sintering (HPS) of a mixture with an elemental atomic ratio corresponding to (Al,Si) 5 (Fe,Ni). The space group was determined to be C 2/ m with Z = 2. The structure model contains three co-occupied sites with occupancy ratios of Si:Al = 0.679:0.321, Ni:Fe = 0.46:0.54 and Ni:Fe = 0.94:0.06, and five sites with full occupancy of Al atoms.
- 21 November 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (11)
Open Access(Al 13.28 Si 2.72 )(Fe 1.19 Ni 2.81 )
The intermetallic phase (Al 13.28 Si 2.72 )(Fe 1.19 Ni 2.81 ) was obtained by high-pressure sintering (HPS) of a mixture with an elemental atomic ratio corresponding to (Al,Si) 5 (Fe,Ni). The space group was determined to be C 2/ m with Z = 2. The structure model contains three co-occupied sites with occupancy ratios of Si:Al = 0.679:0.321, Ni:Fe = 0.46:0.54 and Ni:Fe = 0.94:0.06, and five sites with full occupancy of Al atoms.
- 10 October 2025
- Published by IOP Publishing in Modelling and Simulation in Materials Science and Engineering
- Vol. 33 (7) , 075009
Unveiling the pressure-induced strengthening mechanism in Mg17Al12: a first-principles study on electronic structure and mechanical properties
Magnesium alloys hold significant application value in transportation light weighting, yet the intrinsic strengthening mechanism of their core strengthening phase Mg17Al12 within the high-pressure solidification (HPS) process window remains unclear. Through density functional theory multiscale simulations under 4 GPa, this study reveals the electronic-mechanical coupling mechanism of Mg17Al12, demonstrating that hydrostatic pressure induces lattice contraction to 10.29 Å (Δ = −2.3%) and reduces cohesive energy to −162.49 kJ mol−1, with phonon spectrum confirming high-pressure stability. Material axial stiffness (C11) and shear modulus (C44) increase by 17% and 16%, respectively, achieving a theoretical strength of 9.41 GPa (46% increase) and a 13.7% enhancement in plastic elongation, thereby realizing a synergistic breakthrough in strength and toughness. Electronic structure analysis identifies s–p orbital hybridization of Al bonds triggering a three-dimensional covalent network, while the coexistence of charge localization at Al sites and free electron gas in Mg–Mg bonds establishes a metal-covalent dual-phase ground state, evidenced by reduced Fermi-level density of states and band broadening that reflect dual electron configuration with coexisting localized and itinerant states. Further electronic reconstruction through covalent network strengthening, brittle index optimization (G/B ratio decrease of 8%), and band discretization defines a cross-scale interaction paradigm of ‘quantum orbital modulation → mesoscopic bond reorganization → macroscopic property response’. These findings provide theoretical guidance for HPS parameter design and high-performance magnesium alloy development, advancing lightweight material design toward electronic engineering principles.
- 10 October 2025
- Published by IOP Publishing in Modelling and Simulation in Materials Science and Engineering
- Vol. 33 (7) , 075009
Unveiling the pressure-induced strengthening mechanism in Mg17Al12: a first-principles study on electronic structure and mechanical properties
Magnesium alloys hold significant application value in transportation light weighting, yet the intrinsic strengthening mechanism of their core strengthening phase Mg17Al12 within the high-pressure solidification (HPS) process window remains unclear. Through density functional theory multiscale simulations under 4 GPa, this study reveals the electronic-mechanical coupling mechanism of Mg17Al12, demonstrating that hydrostatic pressure induces lattice contraction to 10.29 Å (Δ = −2.3%) and reduces cohesive energy to −162.49 kJ mol−1, with phonon spectrum confirming high-pressure stability. Material axial stiffness (C11) and shear modulus (C44) increase by 17% and 16%, respectively, achieving a theoretical strength of 9.41 GPa (46% increase) and a 13.7% enhancement in plastic elongation, thereby realizing a synergistic breakthrough in strength and toughness. Electronic structure analysis identifies s–p orbital hybridization of Al bonds triggering a three-dimensional covalent network, while the coexistence of charge localization at Al sites and free electron gas in Mg–Mg bonds establishes a metal-covalent dual-phase ground state, evidenced by reduced Fermi-level density of states and band broadening that reflect dual electron configuration with coexisting localized and itinerant states. Further electronic reconstruction through covalent network strengthening, brittle index optimization (G/B ratio decrease of 8%), and band discretization defines a cross-scale interaction paradigm of ‘quantum orbital modulation → mesoscopic bond reorganization → macroscopic property response’. These findings provide theoretical guidance for HPS parameter design and high-performance magnesium alloy development, advancing lightweight material design toward electronic engineering principles.
- Open Access
- 5 September 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (9) , x250770
Magnesium aluminium zinc gallium, Mg61.81Al12.77Zn61.41Ga24
The title single-crystal was obtained during the synthesis of a Mg–Al–Zn–Ga alloy, which was achieved by subjecting the alloy to elevated pressures and temperatures. The compound crystallizes in the space group Im 3 (No. 204), with seven distinct metal-atom sites. One of these is occupied by gallium, two by aluminium and zinc, one by zinc and magnesium, and three by magnesium. The structure model contains a vacancy-centred Bergman cluster and a 26-face polyhedron centred on one of the magnesium sites. The crystal structure framework in this study shows a marked similarity to previously examined frameworks, but also evinces significant differences [Edagawa et al. (1992). Philos. Mag. B 65, 1011–1023].
- 5 September 2025
- Published by International Union of Crystallography (IUCr) in IUCrData
- Vol. 10 (9) , x250770
Open AccessMagnesium aluminium zinc gallium, Mg61.81Al12.77Zn61.41Ga24
The title single-crystal was obtained during the synthesis of a Mg–Al–Zn–Ga alloy, which was achieved by subjecting the alloy to elevated pressures and temperatures. The compound crystallizes in the space group Im 3 (No. 204), with seven distinct metal-atom sites. One of these is occupied by gallium, two by aluminium and zinc, one by zinc and magnesium, and three by magnesium. The structure model contains a vacancy-centred Bergman cluster and a 26-face polyhedron centred on one of the magnesium sites. The crystal structure framework in this study shows a marked similarity to previously examined frameworks, but also evinces significant differences [Edagawa et al. (1992). Philos. Mag. B 65, 1011–1023].