<?xml version="1.1" encoding="utf-8"?>
<article xsi:noNamespaceSchemaLocation="http://jats.nlm.nih.gov/publishing/1.1/xsd/JATS-journalpublishing1-mathml3.xsd" dtd-version="1.1" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"><front><journal-meta><journal-id journal-id-type="publisher-id">ETR</journal-id><journal-title-group><journal-title>Educational Theory and Research</journal-title></journal-title-group><issn>2995-3448</issn><eissn>2995-3456</eissn><publisher><publisher-name>Art and Technology</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.61369/ETR.2026120002</article-id><article-categories><subj-group subj-group-type="heading"><subject>Article</subject></subj-group></article-categories><title>石墨烯 /2D-hBN 异质结构强耦合机制融入半导体物理课程的教学实践</title><url>https://artdesignp.com/journal/ETR/4/12/10.61369/ETR.2026120002</url><author>黄加耀,黄春栩,谢嘉宁</author><pub-date pub-type="publication-year"><year>2026</year></pub-date><volume>4</volume><issue>12</issue><history><date date-type="pub"><published-time>2026-03-20</published-time></date></history><abstract>半导体物理是光源与照明、光电信息科学与工程等专业本科人才培养中的核心课程，对于学生建立半导体能带结构、载流子输运规律和界面物理等基本理论框架具有重要作用。但在实际教学过程中，普遍存在理论内容抽象、知识体系跨度较大以及课堂教学与科研前沿结合不够紧密等问题。针对上述问题，本文以石墨烯/ 二维hBN 异质结构中的强耦合机制为切入点，探索将前沿科研成果融入半导体物理课程教学的改革路径。结合相关研究进展，构建了理论讲解、数值计算与仿真实践于一体的教学内容体系，将MATLAB 数值计算和严格耦合波分析（RCWA）方法引入课程教学，形成&amp;ldquo;基础理论&amp;mdash; 前沿案例&amp;mdash; 仿真分析&amp;mdash; 能力提升&amp;rdquo;的教学实施模式。同时，借助学习分析方法，对教学改革实施效果进行系统评价。结果表明，该教学实践有助于增强学生的工程实践能力、科研素养和创新意识，为半导体物理课程教学改革提供了可借鉴的思路与参考。</abstract><keywords>半导体物理,2D-hBN 异质结构,强耦合机制,严格耦合波分析方法</keywords></article-meta></front><body/><back><ref-list><ref id="B1" content-type="article"><label>1</label><element-citation publication-type="journal"><p>[1] 李安明, 张红卫, 王俊利, 唐亚楠, 等. " 新工科" 背景下地方应用型高校" 半导体物理" 课程教学改革研究[J]. 工业和信息化教育,2024:11-15.[2] 卢宏, 张玉亭. 基于OBE 理念的' 半导体物理学' 多元化教学模式改革[J]. 科教文汇,2022:45&amp;ndash;48.[3]A. T. Costa, M. I. Vasilevskiy, J. Fern&amp;aacute;ndez-Rossier, and N. M. R. Peres, "Strongly Coupled Magnon&amp;ndash;Plasmon Polaritons in Graphene-Two-Dimensional Ferromagnet Heterostructures," Nano Lett.,pp. 4510&amp;ndash;4515, 2023.[4]Y. Wu et al., "Emerging probing perspective of two-dimensional materials physics: terahertz emission spectroscopy," Light Sci. Appl.,pp. 146, 2024.[5]T. Yang, G.-Q. Wang, Y.-Q. Dai, X.-H. Zheng, X.-J. Ye, and C.-S. Liu, "Two-Dimensional TOD-Graphene in a Honeycomb&amp;ndash;Kagome Lattice: A High- Performance Anode Material for Potassium-Ion Batteries," J. Phys. Chem. C,pp. 9413&amp;ndash;9421, 2024.[6]A. K. Geim and K. S. Novoselov, "The rise of graphene," Nat. Mater.,pp. 183&amp;ndash;191, 2007.[7]J. Olivo, H. Ferrari, and M. Cuevas, "Surface recoil force on dielectric nanoparticle enhancement via graphene acoustic surface plasmon excitation: nonlocal effect consideration," Opt. Lett.,pp. 1249, 2024.[8]H. Lu, X. Gan, D. Mao, and J. Zhao, "Graphene-supported manipulation of surface plasmon polaritons in metallic nanowaveguides," Photonics Res., pp. 162, 2017.[9]G. W. Hanson, "Dyadic Green's functions and guided surface waves for a surface conductivity model of graphene," J. Appl. Phys., 2008.[10]Y. M. Qing, H. F. Ma, and T. J. Cui, "Theoretical Analysis of Tunable Multimode Coupling in a Grating-Assisted Double-Layer Graphene Plasmonic System," ACS Photonics, pp. 2884&amp;ndash;2893, 2019.[11]M. Chen et al., "Van der Waals isotope heterostructures for engineering phonon polariton dispersions," Nat. Commun., pp. 4782, 2023.[12]K. Zhang, Y. Feng, F. Wang, Z. Yang, and J. Wang, "Two dimensional hexagonal boron nitride (2D-hBN): synthesis, properties and applications," J. Mater. Chem. C, pp. 11992&amp;ndash;12022, 2017.[13]H. Arianfard, J. Wu, S. Juodkazis, and D. J. Moss, "Optical Analogs of Rabi Splitting in Integrated Waveguide ‐Coupled Resonators," Adv. Phys. Res. (2023).[14]M. G. Moharam and T. K. Gaylord, "Rigorous coupled-wave analysis of planargrating diffraction," J. Opt. Soc. Am., pp. 811, 1981.[15]K. Ziegler, "Minimal conductivity of graphene: Nonuniversal values from the Kubo formula," Phys. Rev. B, pp. 233407, 2007.[16]A. Kumar, D. Solanki, K. Watanabe, T. Taniguchi, A. K. Sood, and A. Das,"Interlayer Phonon Coupling and Enhanced Electron&amp;ndash;Phonon Interactions in Doubly Aligned hBN/Graphene/hBN Heterostructures," ACS Nano, pp. 16415&amp;ndash;16423, 2025.[17]B. Gil, G. Cassabois, R. Cusco, G. Fugallo, and L. Artus, "Boron nitride for excitonics, nano photonics, and quantum technologies," Nanophotonics, pp. 3483&amp;ndash;3504, 2020.[18]B. Zhao, J.-H. Song, M. Brongersma, and S. Fan, "Atomic-Scale Control of Coherent Thermal Radiation," ACS Photonics, pp. 872&amp;ndash;878, 2021.[19]B. Zhao and Z. M. Zhang, "Strong Plasmonic Coupling between Graphene Ribbon Array and Metal Gratings," ACS Photonics, pp. 1611&amp;ndash;1618, 2015.[20]Y. Shi, W. Li, A. Raman, and S. Fan, "Optimization of Multilayer Optical Films with a Memetic Algorithm and Mixed Integer Programming," ACS Photonics, pp. 684&amp;ndash;691, 2018.[21]Y. M. Qing, H. F. Ma, and T. J. Cui, "Investigation of strong multimode interaction in a graphene-based hybrid coupled plasmonic system," Carbon N. Y. pp. 596&amp;ndash;602, 2019.[22]L. Qiu, D. Li, and H.-M. Cheng, "Structural Control of Graphene-Based Materials for Unprecedented Performance," ACS Nano, pp. 5085&amp;ndash;5092, 2018.[23]J. Huang, F. Deng, F. Ye, H. Y. Fu, S. Zhang, and Q. Li, "Strong plasmon - phonon coupling for graphene/ hBN thermal emitter atomic system," Carbon N. Y., pp. 118210, 2023.[24]D. S. Dovzhenko, S. V. Ryabchuk, Y. P. Rakovich, and I. R. Nabiev, "Light&amp;ndash; matter interaction in the strong coupling regime: configurations, conditions, and applications," Nanoscale, pp. 3589&amp;ndash;3605, 2018.</p><pub-id pub-id-type="doi"/></element-citation></ref></ref-list></back></article>
