Structure-dependentElectron–Phonon Couplingand Superconductivity in Two-dimensional MB7 (M = Cr, Mn,Fe) Monolayers
Abstract We present a systematic first-principles study of two-dimensional MB7 (M = Cr, Mn, Fe) monolayers, focusing on their structural, electronic, vibrational, and superconducting properties. CrB7 and FeB7 exhibit transition-metal-stabilized boron frameworks, consisting of a distorted hexagonal boron layer sandwiched between two kagome boron layers, where the structural stability is enhanced by charge transfer from transition-metal atoms. Phonon calculations demonstrate that CrB7 is dynamically stable, whereas FeB7 exhibits only a weak soft mode associated with the intrinsic flexibility of two-dimensional systems.In contrast, the high-symmetry MnB7 structure exhibits phonon instability and spontaneously reconstructs into a lower-energy monoclinic MnB7 phase. Based on the dynamically stable structures and the reconstructed monoclinic phase, we further investigate their phonon-mediated superconducting properties. All investigated stable and reconstructed phases exhibit phonon-mediated superconductivity, with electron–phonon coupling (EPC) primarily originating from low-frequency metal-associated phonon modes. These results reveal the crucial roles of structural stability, electronic states, and phonon characteristics in regulating superconductivity in two-dimensional transition-metal borides, providing insights into the design of low-dimensional boron-based superconducting materials.
Authors
- Xin Qu (ORCID: https://orcid.org/0000-0003-4540-5557)
- Wanting Han (ORCID: https://orcid.org/0000-0002-2173-3647)
- Han Fu
Institutions
- Jilin Normal University (CN)
- Jilin University (CN)
- Jilin Engineering Normal University (CN)
- Jilin Medical University (CN)
Publication Details
- Journal
- The Journal of Physical Chemistry C
- Published
- 2026-08-14
- DOI
- https://doi.org/10.1021/acs.jpcc.6c01930
- Primary Topic
- Boron and Carbon Nanomaterials Research
- Type
- article
- Field-Weighted Citation Impact
- 0.00