Article(id=1319726411213034077, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726382268138030, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20250107, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1739894400000, receivedDateStr=2025-02-19, revisedDate=1741449600000, revisedDateStr=2025-03-09, acceptedDate=null, acceptedDateStr=null, onlineDate=1792576895764, onlineDateStr=2026-10-21, pubDate=1763568000000, pubDateStr=2025-11-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792576895764, onlineIssueDateStr=2026-10-21, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792576895764, creator=13701087609, updateTime=1792576895764, updator=13701087609, issue=Issue{id=1319726382268138030, tenantId=1146029695717560320, journalId=1263187385517883426, year='2025', volume='53', issue='11', pageStart='3079', pageEnd='3432', issueExtLink='null', onlineDate='null', pubDate='1763568000000', pubDateStr='2025-11-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792576888863, creator='13701087609', updateTime=1792577494231, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1319728921399116056, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726382268138030, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1319728921403310361, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726382268138030, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=3339, endPage=3351, ext={EN=ArticleExt(id=1319726411414360670, articleId=1319726411213034077, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Effect of B and Al co-Doping on Single-Crystal Morphology and Electrochemical Property of Spinel LiMn2O4, columnId=1319726165087077079, journalTitle=Journal of the Chinese Ceramic Society, columnName=Research Article, runingTitle=null, highlight=null, articleAbstract=
Introduction

Rechargeable lithium-ion batteries (LIBs) are critical energy storage devices widely used in smartphones, electric vehicles, and hybrid vehicles due to their high efficiency and versatility. Spinel LiMn2O4 stands out as a promising cathode material owing to its eco-friendliness, safety, and cost-effectiveness. However, its practical application is limited by rapid capacity fading during cycling, especially under high current densities or elevated temperatures (55 ℃), caused by Jahn-Teller (J-T) distortion, Mn3+ dissolution, and oxygen defects. To address these issues, doping LiMn2O4 with elements like Al3+, B3+, Ni2+, or Mg2+ is a common strategy to stabilize Mn's average oxidation state (+3.5) and suppress J-T distortion. Concurrently, crystal facet engineering optimizes performance: truncated octahedral particles with dominant (111) facets (low surface energy, dense Mn packing) minimize Mn dissolution, while (100)/(110) facets enhance Li+ mobility for improved rate capability. Combining doping and facet control has emerged as a key research focus. For instance, B-doped LiMn1.96B0.06O4 exhibited 110.3 mA·h·g-1 at 5.0 C with 51.8% capacity retention after 2000 cycles, outperforming undoped LiMn2O4. Ni—B co-doping further refined morphology and boosted retention to 70.6%. Similarly, Mg—Al co-doped LiMg0.03Al0.10Mn1.87O4 retained 76.2% capacity after 1000 cycles at 10.0 C, while Zn—Al doping achieved 70%-75% retention over 2000 cycles. These studies highlight how doping regulates crystal growth, favoring truncated octahedral morphologies with balanced stability and kinetics. Building on this, our work synthesizes LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) via solid-state combustion to study Al doping's impact. Results reveal that Al content modulates facet growth: low doping levels yield two-facet (111/100) truncated octahedrons, while higher doping introduces (110) facets, ultimately leading to quasi-spherical particles. This controlled facet producing strategy is designed to optimize structural stability and electrochemical performance for advanced LIBs.

Methods

LiB0.08Mn1.92O4 and LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) were synthesized by stoichiometric mixing of Li2CO3, H3BO3, MnCO3, and Al(OH)(CH3COO)2 (total 30 g) with 1.5 g citric acid as a combustion agent. The mixture was ball-milled in ethanol for 10 h, dried, and calcined at 500 ℃ for 1 h. After grinding, it was sintered at 650 ℃ for 6 h. Products were labeled as B0.08 and B0.08Aly. Cathode slurry was prepared by blending active material, carbon black, and PVDF (8∶1∶1) with NMP solvent, followed by 30 min ball milling. The slurry was coated onto Al foil, dried at 80 ℃ for 4 h, and cut into 14 mm discs (active material loading: about 1.0 mg/cm2). CR2032 coin cells were assembled in an Ar-filled glovebox using Li metal anode, LiPF6 electrolyte (1.0 M in EC/DMC/EMC), and Celgard 2320 separator. Material phases were analyzed via XRD (Cu Kα, 10°-80°). Morphology and microstructure were examined by FE-SEM and TEM. Surface composition and valence states were determined via XPS. Electrochemical tests (Land CT2001A) included cycling (25/55 ℃, 3.0-4.5 V) and rate performance. CV and EIS were conducted using a CHI604D workstation.

Results and discussion

XRD analysis confirmed that B0.08 and B—Al co-doped samples crystallized in the spinel LiMn2O4 structure (). B—Al co-doping enhanced crystallinity, with diffraction peaks intensifying until y(Al)≥0.06, beyond which crystallinity declined. A lattice contraction was observed via (400) peak shifts, attributed to smaller B3+/Al3+(0.0400/0.0535 nm) replacing Mn3+(0.0645 nm) and shorter B/Al—O bonds, suppressing J-T distortion. SEM revealed that B—Al co-doping refined particle uniformity and morphology: B0.08Al0.02 exhibited truncated octahedral single-crystals with high (111) and minor (100)/(110) facets, while higher Al content (y≥0.04) led to spherical polyhedrons due to reduced facet growth rates. TEM/SAED confirmed improved crystallinity for B0.08Al0.02, with distinct lattice fringes (0.476 nm for (111)) and ordered diffraction patterns. XPS verified B3+/Al3+ incorporation and a higher Mn4+ ratio (B0.08Al0.02∶ Mn3+/Mn4+=47.29%/52.71%), stabilizing the Mn—O framework. Electrochemical tests demonstrated superior performance for B0.08Al0.02∶ At 5.0 C, it retained 83.9% capacity after 500 cycles (vs. 71.3% for B0.08) due to suppressed Mn dissolution and enhanced Li+ transport from truncated octahedral morphology. High-rate testing (15.0 C, 20.0 C) showed B0.08Al0.02 retained 77.2% capacity after 500 cycles, outperforming B0.08 (58.2%). Elevated-temperature (55 ℃) cycling revealed B0.08Al0.02 maintained 70% capacity retention (200 cycles), attributed to reduced side reactions and structural stability. CV and EIS confirmed faster Li+ diffusion (DLi+: 3.14×10-11 cm2·s-1) and lower charge-transfer resistance for B0.08Al0.02. Kinetic analysis showed a lower activation energy (24.76 kJ/mol vs. 28.53 kJ/mol for B0.08), indicating an enhanced reaction kinetics.

Conclusions

B—Al co-doped LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) cathode materials were synthesized via solid-phase combustion. B—Al co-doping enhanced crystal growth and facet evolution: particles transitioned from truncated octahedrons with two facets (111, 100) to those incorporating (111), (100), and (110) facets as Al content increased. At y(Al)≥0.04, spherical-like polyhedrons dominated. The optimized LiB0.08Al0.02Mn1.90O4 (B0.08Al0.02) exhibited superior crystallinity and well-defined truncated octahedral single-crystals. B0.08Al0.02 demonstrated exceptional rate capability and cycling stability. At 1.0 C, 5.0 C, 10.0 C, 15.0 C, 20.0 C, and 55 ℃/5.0 C, initial discharge capacities reached 114.7, 102.8, 86.3, 82.6, 75.3, and 107.4 mA·h·g-1, respectively. After 500 cycles, capacity retention rates were 83.9% (5.0 C), 81.9% (10 C), 90.3% (15.0 C), 77.2% (20.0 C), and 62.0% (55 ℃/5.0 C), outperforming other samples. CV and EIS analyses demonstrated superior electrochemical properties for the B0.08Al0.02, including a higher Li+ diffusion coefficient (3.14×10-11 cm2·s-1), a lower apparent activation energy (24.76 kJ/mol), and a reduced charge-transfer resistance (114.2 Ω). These results indicate enhanced Li+ transport kinetics and improved structural stability.

, authors=Long SHI1, Yongsheng YANG1, Yuxu LUO2, Junming GUO1, Kaikun WANG3, authorsList=Long SHI, Yongsheng YANG, Yuxu LUO, Junming GUO, Kaikun WANG, authorCompany=null, correspAuthors=Yongsheng YANG, Junming GUO, authorNote=

SHI Long (1984-), male, Ph.D., Associate Professor. E-mail:

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YANG Yongsheng (1971-), male, Ph.D., Associate Professor. E-mail: ;
GUO Junming (1962-), male, Master, Professor.
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为改善尖晶石LiMn2O4的循环稳定性,抑制其容量衰减,采用固相燃烧法合成了B—Al共掺截断八面体形貌LiB0.08AlyMn1.92-yO4(y=0.01、0.02、0.04、0.06和0.08)正极材料。结果表明,B—Al复合掺杂没有改变LiMn2O4的立方尖晶石结构,但可显著影响其晶面生长速率,促进材料的晶体生长和晶面的择优生长,且颗粒尺寸增大。在B—Al共掺杂中随Al掺杂量增加,颗粒形貌由包含(111)和(100)2个晶面的截断八面体逐渐形成包含(111)、(100)和(110)3个晶面的单晶截断八面体,y(Al)≥0.04时形成类球形颗粒,其中,LiB0.08Al0.02Mn1.90O4样品形成3个晶面的完整单晶截断八面体形貌颗粒,具有优良的倍率性能和长循环稳定性。在室温1.0、10.0、15.0 C倍率和高温(55 ℃)1.0 C倍率下,其初始放电比容量分别为114.7、86.3、82.6 mA·h·g-1和114.7 mA·h·g-1;1.0 C倍率200次循环、10.0 C和15.0 C倍率500次循环以及高温(55 ℃)1.0 C倍率200次循环后,容量保持率分别为84.7%、81.9%、90.3%和70.0%。LiB0.08Al0.02Mn1.90O4电极材料具有较大的锂离子扩散系数(3.14×10-11 cm2·s-1)以及相对较小的表观活化能(24.76 kJ/mol)和电荷转移阻抗(114.2 Ω),有利于锂离子的输运。B—Al共掺杂和单晶截断八面体形貌抑制了Jahn-Teller畸变并缓解Mn的溶解,提高了尖晶石型LiMn2O4正极材料的晶体结构稳定性,增强了材料的高倍率性能和长循环稳定性。

, authors=时龙1, 杨永胜1, 罗宇旭2, 郭俊明1, 王开坤3, authorsList=时龙, 杨永胜, 罗宇旭, 郭俊明, 王开坤, authorCompany=null, correspAuthors=杨永胜, 郭俊明, authorNote=

时龙(1984—),男,博士,副教授。

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杨永胜(1971—),男,博士,副教授;
郭俊明(1962—),男,硕士,教授。
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B和Al复合掺杂对尖晶石型LiMn2O4单晶形貌及电化学性能的影响
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时龙 1 , 杨永胜 1 , 罗宇旭 2 , 郭俊明 1 , 王开坤 3
硅酸盐学报 | 研究论文 2025,53(11): 3339-3351
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硅酸盐学报 |研究论文 2025 , 53 (11) : 3339 -3351
B和Al复合掺杂对尖晶石型LiMn2O4单晶形貌及电化学性能的影响
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时龙(1984—),男,博士,副教授。

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时龙1 , 杨永胜1 , 罗宇旭2, 郭俊明1 , 王开坤3
作者信息
  • 1.昭通学院化学化工学院,云南 昭通 657000
  • 2.云南民族大学化学与环境学院,昆明 650500
  • 3.北京科技大学材料科学与工程学院,北京 100083
通讯作者:
杨永胜(1971—),男,博士,副教授;
郭俊明(1962—),男,硕士,教授。
作者简介:

时龙(1984—),男,博士,副教授。

Effect of B and Al co-Doping on Single-Crystal Morphology and Electrochemical Property of Spinel LiMn2O4
Long SHI1 , Yongsheng YANG1 , Yuxu LUO2, Junming GUO1 , Kaikun WANG3
Affiliations
  • 1.School of Chemistry and Chemical Engineering, Zhaotong University, Zhaotong 657000, Yunnan, China
  • 2.School of Chemistry and Environment, Yunnan Minzu University, Kunming 650500, China
  • 3.School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China
  • Corresponding Author:
    YANG Yongsheng (1971-), male, Ph.D., Associate Professor. E-mail: ;
    GUO Junming (1962-), male, Master, Professor.

    SHI Long (1984-), male, Ph.D., Associate Professor. E-mail:

出版时间: 2025-11-20 doi: 10.14062/j.issn.0454-5648.20250107
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为改善尖晶石LiMn2O4的循环稳定性,抑制其容量衰减,采用固相燃烧法合成了B—Al共掺截断八面体形貌LiB0.08AlyMn1.92-yO4(y=0.01、0.02、0.04、0.06和0.08)正极材料。结果表明,B—Al复合掺杂没有改变LiMn2O4的立方尖晶石结构,但可显著影响其晶面生长速率,促进材料的晶体生长和晶面的择优生长,且颗粒尺寸增大。在B—Al共掺杂中随Al掺杂量增加,颗粒形貌由包含(111)和(100)2个晶面的截断八面体逐渐形成包含(111)、(100)和(110)3个晶面的单晶截断八面体,y(Al)≥0.04时形成类球形颗粒,其中,LiB0.08Al0.02Mn1.90O4样品形成3个晶面的完整单晶截断八面体形貌颗粒,具有优良的倍率性能和长循环稳定性。在室温1.0、10.0、15.0 C倍率和高温(55 ℃)1.0 C倍率下,其初始放电比容量分别为114.7、86.3、82.6 mA·h·g-1和114.7 mA·h·g-1;1.0 C倍率200次循环、10.0 C和15.0 C倍率500次循环以及高温(55 ℃)1.0 C倍率200次循环后,容量保持率分别为84.7%、81.9%、90.3%和70.0%。LiB0.08Al0.02Mn1.90O4电极材料具有较大的锂离子扩散系数(3.14×10-11 cm2·s-1)以及相对较小的表观活化能(24.76 kJ/mol)和电荷转移阻抗(114.2 Ω),有利于锂离子的输运。B—Al共掺杂和单晶截断八面体形貌抑制了Jahn-Teller畸变并缓解Mn的溶解,提高了尖晶石型LiMn2O4正极材料的晶体结构稳定性,增强了材料的高倍率性能和长循环稳定性。

尖晶石锰酸锂  /  硼铝共掺杂  /  正极材料  /  截断八面体  /  晶面调控
Introduction

Rechargeable lithium-ion batteries (LIBs) are critical energy storage devices widely used in smartphones, electric vehicles, and hybrid vehicles due to their high efficiency and versatility. Spinel LiMn2O4 stands out as a promising cathode material owing to its eco-friendliness, safety, and cost-effectiveness. However, its practical application is limited by rapid capacity fading during cycling, especially under high current densities or elevated temperatures (55 ℃), caused by Jahn-Teller (J-T) distortion, Mn3+ dissolution, and oxygen defects. To address these issues, doping LiMn2O4 with elements like Al3+, B3+, Ni2+, or Mg2+ is a common strategy to stabilize Mn's average oxidation state (+3.5) and suppress J-T distortion. Concurrently, crystal facet engineering optimizes performance: truncated octahedral particles with dominant (111) facets (low surface energy, dense Mn packing) minimize Mn dissolution, while (100)/(110) facets enhance Li+ mobility for improved rate capability. Combining doping and facet control has emerged as a key research focus. For instance, B-doped LiMn1.96B0.06O4 exhibited 110.3 mA·h·g-1 at 5.0 C with 51.8% capacity retention after 2000 cycles, outperforming undoped LiMn2O4. Ni—B co-doping further refined morphology and boosted retention to 70.6%. Similarly, Mg—Al co-doped LiMg0.03Al0.10Mn1.87O4 retained 76.2% capacity after 1000 cycles at 10.0 C, while Zn—Al doping achieved 70%-75% retention over 2000 cycles. These studies highlight how doping regulates crystal growth, favoring truncated octahedral morphologies with balanced stability and kinetics. Building on this, our work synthesizes LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) via solid-state combustion to study Al doping's impact. Results reveal that Al content modulates facet growth: low doping levels yield two-facet (111/100) truncated octahedrons, while higher doping introduces (110) facets, ultimately leading to quasi-spherical particles. This controlled facet producing strategy is designed to optimize structural stability and electrochemical performance for advanced LIBs.

Methods

LiB0.08Mn1.92O4 and LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) were synthesized by stoichiometric mixing of Li2CO3, H3BO3, MnCO3, and Al(OH)(CH3COO)2 (total 30 g) with 1.5 g citric acid as a combustion agent. The mixture was ball-milled in ethanol for 10 h, dried, and calcined at 500 ℃ for 1 h. After grinding, it was sintered at 650 ℃ for 6 h. Products were labeled as B0.08 and B0.08Aly. Cathode slurry was prepared by blending active material, carbon black, and PVDF (8∶1∶1) with NMP solvent, followed by 30 min ball milling. The slurry was coated onto Al foil, dried at 80 ℃ for 4 h, and cut into 14 mm discs (active material loading: about 1.0 mg/cm2). CR2032 coin cells were assembled in an Ar-filled glovebox using Li metal anode, LiPF6 electrolyte (1.0 M in EC/DMC/EMC), and Celgard 2320 separator. Material phases were analyzed via XRD (Cu Kα, 10°-80°). Morphology and microstructure were examined by FE-SEM and TEM. Surface composition and valence states were determined via XPS. Electrochemical tests (Land CT2001A) included cycling (25/55 ℃, 3.0-4.5 V) and rate performance. CV and EIS were conducted using a CHI604D workstation.

Results and discussion

XRD analysis confirmed that B0.08 and B—Al co-doped samples crystallized in the spinel LiMn2O4 structure (). B—Al co-doping enhanced crystallinity, with diffraction peaks intensifying until y(Al)≥0.06, beyond which crystallinity declined. A lattice contraction was observed via (400) peak shifts, attributed to smaller B3+/Al3+(0.0400/0.0535 nm) replacing Mn3+(0.0645 nm) and shorter B/Al—O bonds, suppressing J-T distortion. SEM revealed that B—Al co-doping refined particle uniformity and morphology: B0.08Al0.02 exhibited truncated octahedral single-crystals with high (111) and minor (100)/(110) facets, while higher Al content (y≥0.04) led to spherical polyhedrons due to reduced facet growth rates. TEM/SAED confirmed improved crystallinity for B0.08Al0.02, with distinct lattice fringes (0.476 nm for (111)) and ordered diffraction patterns. XPS verified B3+/Al3+ incorporation and a higher Mn4+ ratio (B0.08Al0.02∶ Mn3+/Mn4+=47.29%/52.71%), stabilizing the Mn—O framework. Electrochemical tests demonstrated superior performance for B0.08Al0.02∶ At 5.0 C, it retained 83.9% capacity after 500 cycles (vs. 71.3% for B0.08) due to suppressed Mn dissolution and enhanced Li+ transport from truncated octahedral morphology. High-rate testing (15.0 C, 20.0 C) showed B0.08Al0.02 retained 77.2% capacity after 500 cycles, outperforming B0.08 (58.2%). Elevated-temperature (55 ℃) cycling revealed B0.08Al0.02 maintained 70% capacity retention (200 cycles), attributed to reduced side reactions and structural stability. CV and EIS confirmed faster Li+ diffusion (DLi+: 3.14×10-11 cm2·s-1) and lower charge-transfer resistance for B0.08Al0.02. Kinetic analysis showed a lower activation energy (24.76 kJ/mol vs. 28.53 kJ/mol for B0.08), indicating an enhanced reaction kinetics.

Conclusions

B—Al co-doped LiB0.08AlyMn1.92-yO4 (y=0.01, 0.02, 0.04, 0.06, 0.08) cathode materials were synthesized via solid-phase combustion. B—Al co-doping enhanced crystal growth and facet evolution: particles transitioned from truncated octahedrons with two facets (111, 100) to those incorporating (111), (100), and (110) facets as Al content increased. At y(Al)≥0.04, spherical-like polyhedrons dominated. The optimized LiB0.08Al0.02Mn1.90O4 (B0.08Al0.02) exhibited superior crystallinity and well-defined truncated octahedral single-crystals. B0.08Al0.02 demonstrated exceptional rate capability and cycling stability. At 1.0 C, 5.0 C, 10.0 C, 15.0 C, 20.0 C, and 55 ℃/5.0 C, initial discharge capacities reached 114.7, 102.8, 86.3, 82.6, 75.3, and 107.4 mA·h·g-1, respectively. After 500 cycles, capacity retention rates were 83.9% (5.0 C), 81.9% (10 C), 90.3% (15.0 C), 77.2% (20.0 C), and 62.0% (55 ℃/5.0 C), outperforming other samples. CV and EIS analyses demonstrated superior electrochemical properties for the B0.08Al0.02, including a higher Li+ diffusion coefficient (3.14×10-11 cm2·s-1), a lower apparent activation energy (24.76 kJ/mol), and a reduced charge-transfer resistance (114.2 Ω). These results indicate enhanced Li+ transport kinetics and improved structural stability.

spinel lithium manganese oxide  /  boron-aluminum co-doping  /  cathode material  /  truncated octahedron  /  crystal plane regulation
时龙, 杨永胜, 罗宇旭, 郭俊明, 王开坤. B和Al复合掺杂对尖晶石型LiMn2O4单晶形貌及电化学性能的影响. 硅酸盐学报, 2025 , 53 (11) : 3339 -3351 . DOI: 10.14062/j.issn.0454-5648.20250107
Long SHI, Yongsheng YANG, Yuxu LUO, Junming GUO, Kaikun WANG. Effect of B and Al co-Doping on Single-Crystal Morphology and Electrochemical Property of Spinel LiMn2O4[J]. Journal of the Chinese Ceramic Society, 2025 , 53 (11) : 3339 -3351 . DOI: 10.14062/j.issn.0454-5648.20250107
  • 国家自然科学基金(51972282)
  • 云南省院士(专家)工作站项目(202405AF140034)
  • 昭通学院博士科研启动经费项目
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doi: 10.14062/j.issn.0454-5648.20250107
  • 接收时间:2025-02-19
  • 首发时间:2026-10-21
  • 出版时间:2025-11-20
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  • 收稿日期:2025-02-19
  • 修回日期:2025-03-09
基金
国家自然科学基金(51972282)
云南省院士(专家)工作站项目(202405AF140034)
昭通学院博士科研启动经费项目
作者信息
    1.昭通学院化学化工学院,云南 昭通 657000
    2.云南民族大学化学与环境学院,昆明 650500
    3.北京科技大学材料科学与工程学院,北京 100083

通讯作者:

杨永胜(1971—),男,博士,副教授;
郭俊明(1962—),男,硕士,教授。
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