Please use this identifier to cite or link to this item: https://has.hcu.ac.th/jspui/handle/123456789/2059
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dc.contributor.authorPrayoonsak Pluengphon-
dc.contributor.authorWiwittawin Sukmas-
dc.contributor.authorPrutthipong Tsuppayakorn-aek-
dc.contributor.authorKomsilp Kotmool-
dc.contributor.authorAparporn Sakulkalavek-
dc.contributor.authorBurapat Inceesungvorn-
dc.contributor.authorThiti Bovornratanaraks-
dc.contributor.authorWei Luo-
dc.contributor.authorประยูรศักดิ์ เปลื้องผล-
dc.contributor.authorวิวิธวินท์ สุขมาศ-
dc.contributor.authorพฤทธิพงษ์ ทรัพยากรเอก-
dc.contributor.authorคมศิลป์ โคตมูล-
dc.contributor.authorอาภาภรณ์ สกุลการะเวก-
dc.contributor.authorบูรภัทร์ อินทรีย์สังวร-
dc.contributor.authorธิติ บวรรัตนารักษ์-
dc.contributor.otherHuachiew Chalermprakiet University. Faculty of Science and Technology. Division of Physical Scienceth
dc.contributor.otherChulalongkorn University. Metallurgy and Materials Science Research Instituteth
dc.contributor.otherChulalongkorn University. Faculty of Science. Department of Physicsth
dc.contributor.otherKing Mongkut’s Institute of Technology Ladkrabang. College of Advanced Manufacturing Innovationth
dc.contributor.otherKing Mongkut’s Institute of Technology Ladkrabang. School of Science. Department of Physicsth
dc.contributor.otherChiang Mai University. Faculty of Science. Center of Excellence in Materials Science and Technologyth
dc.contributor.otherChulalongkorn University. Faculty of Science. Department of Physicsth
dc.contributor.otherUppsala University. Department of Physics and Astronomy. Materials Theory Divisionth
dc.date.accessioned2024-04-15T07:35:12Z-
dc.date.available2024-04-15T07:35:12Z-
dc.date.issued2024-
dc.identifier.citationJournal of Physics and Chemistry of Solids 189, (June 2024) : 111948th
dc.identifier.otherhttps://doi.org/10.1016/j.jpcs.2024.111948-
dc.identifier.urihttps://has.hcu.ac.th/jspui/handle/123456789/2059-
dc.descriptionสามารถเข้าถึงบทความฉบับเต็มได้ที่ https://doi.org/10.1016/j.jpcs.2024.111948th
dc.description.abstractThe layered hexagonal compound NaLiC4 has been thoroughly investigated to assess its thermodynamic and dynamic stability in comparison to its parent compounds NaC2and LiC2. Utilizing first-principles calculations and phonon analyses, NaLiC4 has demonstrated remarkable stability within a pressure range of 50 to 100 GPa, surpassing the thermodynamic stability of NaC2and LiC2. It exhibits metallic behavior with distinctive electronic bands along high symmetry paths, suggesting a conducive environment for superconductivity. The superconducting transition temperature (Tc) of NaLiC4under different pressures was estimated using the Allen-Dynes equation, with a maximum Tcof 39 K observed at 50 GPa. However, as pressure increases, Tcgradually decreases, indicating the significant impact of external pressure conditions on the superconducting properties. Notably, the in-plane E2gphonon mode originating from the layered hexagonal structure of carbon atoms plays a crucial role in facilitating electron-phonon coupling and influencing the superconducting behavior and Tcof NaLiC4. These findings highlight the thermodynamic and dynamic stability of NaLiC4as a promising candidate for exploring superconductivity, offering insights into its electronic properties, pressure-dependent Tcbehavior, and the influence of specific phonon modes. Further theoretical investigations and experimental studies are necessary to fully unlock the potential of NaLiC4and its contribution to the development of high-performance superconductorsth
dc.language.isoen_USth
dc.subjectฟิล์มบางth
dc.subjectThin filmsth
dc.subjectตัวนำไฟฟ้ายิ่งยวดอุณหภูมิสูงth
dc.subjectSuperconductivityth
dc.subjectวัสดุที่อุณหภูมิสูงth
dc.subjectMaterials at high temperatureth
dc.titleThermodynamic and dynamic stability of NaLiC : Exploring superconductivity in a layered hexagonal compound through first-principles calculationsth
dc.typeArticleth
Appears in Collections:Science and Technology - Artical Journals

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