Pub Date : 2025-01-24DOI: 10.1140/epjb/s10051-024-00860-8
Ya-Ping Li, Ying-Jie Chen, Meng-Meng Zheng
In recent years, two-dimensional (2D) superconducting materials have garnered significant interest due to their unique properties and potential applications. Here, we conducted thermodynamic and dynamic stability studies on 51 metal-intercalated hexagonal boron carbon (h-BC) compounds, and ultimately identified 22 stable compounds. Among these 22 compounds, 18 materials are metals, while the remaining 4 materials include 1 semiconductor ((hbox {MgB}_{2}hbox {C}_{2})) and 3 semimetals ((hbox {TiB}_{2}hbox {C}_{2}), (hbox {ZrB}_{2}hbox {C}_{2}), and (hbox {HfB}_{2}hbox {C}_{2})). The possible superconductivity of eighteen metals is studied by solving the Allen–Dynes modified McMillan equation to estimate their superconducting transition temperature ((T_{c})). The highest (T_{c}) is observed in (hbox {KB}_{2}hbox {C}_{2}) ((T_{c}) = 53.47 K), followed by (hbox {NaB}_{2}hbox {C}_{2}) ((T_{c}) = 48.30 K), while the lowest (T_{c}) is in (hbox {AlB}_{2}hbox {C}_{2}) ((T_{c}) = 0.04 K). Due to the high (T_{c}) of alkali metal intercalation compounds, this work mainly focuses on them. For alkali metal intercalation compounds, we found that the (T_{c}) rises with the increase of the main group atomic number, mainly due to the degree of metalization of the (sigma )-bonding band at the Fermi level. Another important reason is the softening of the phonon spectrum. These findings enrich the family of 2D superconductors, providing new theoretical insights for experimental synthesis and opening research ideas for 2D superconducting electronic devices.
{"title":"Theoretical study on superconductivity of metal-intercalated boron carbon compounds","authors":"Ya-Ping Li, Ying-Jie Chen, Meng-Meng Zheng","doi":"10.1140/epjb/s10051-024-00860-8","DOIUrl":"10.1140/epjb/s10051-024-00860-8","url":null,"abstract":"<p>In recent years, two-dimensional (2D) superconducting materials have garnered significant interest due to their unique properties and potential applications. Here, we conducted thermodynamic and dynamic stability studies on 51 metal-intercalated hexagonal boron carbon (<i>h</i>-BC) compounds, and ultimately identified 22 stable compounds. Among these 22 compounds, 18 materials are metals, while the remaining 4 materials include 1 semiconductor (<span>(hbox {MgB}_{2}hbox {C}_{2})</span>) and 3 semimetals (<span>(hbox {TiB}_{2}hbox {C}_{2})</span>, <span>(hbox {ZrB}_{2}hbox {C}_{2})</span>, and <span>(hbox {HfB}_{2}hbox {C}_{2})</span>). The possible superconductivity of eighteen metals is studied by solving the Allen–Dynes modified McMillan equation to estimate their superconducting transition temperature (<span>(T_{c})</span>). The highest <span>(T_{c})</span> is observed in <span>(hbox {KB}_{2}hbox {C}_{2})</span> (<span>(T_{c})</span> = 53.47 K), followed by <span>(hbox {NaB}_{2}hbox {C}_{2})</span> (<span>(T_{c})</span> = 48.30 K), while the lowest <span>(T_{c})</span> is in <span>(hbox {AlB}_{2}hbox {C}_{2})</span> (<span>(T_{c})</span> = 0.04 K). Due to the high <span>(T_{c})</span> of alkali metal intercalation compounds, this work mainly focuses on them. For alkali metal intercalation compounds, we found that the <span>(T_{c})</span> rises with the increase of the main group atomic number, mainly due to the degree of metalization of the <span>(sigma )</span>-bonding band at the Fermi level. Another important reason is the softening of the phonon spectrum. These findings enrich the family of 2D superconductors, providing new theoretical insights for experimental synthesis and opening research ideas for 2D superconducting electronic devices.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"98 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-01-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143109380","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-21DOI: 10.1140/epjb/s10051-024-00855-5
Govind Singh, Dinesh Khattar, Neha Agrawal
This paper offers a unique synchronization strategy for synchronizing eight chaotic systems. The new approach is referred to as dual quadratic compound anti synchronization. We additionally employed signal multi-switching to augment the complexity of the suggested technique. In communication theory, the transmission and security of the resulting signal are more effective because of the numerous combinations of chaotic systems and multiswitching that provide such complicated dynamic behavior. To demonstrate the acquired results, Lorenz, Rössler, Lü, and Chen chaotic system are used. Using the Lyapunov stability principle, sufficient conditions are attained and appropriate controllers are built to achieve the required synchronization between eight chaotic systems. To validate the findings from theory, numerical simulations, and graphics are presented using MATLAB.
{"title":"Dual quadratic compound multiswitching anti-synchronization of Lorenz, Rössler, Lü and Chen chaotic systems","authors":"Govind Singh, Dinesh Khattar, Neha Agrawal","doi":"10.1140/epjb/s10051-024-00855-5","DOIUrl":"10.1140/epjb/s10051-024-00855-5","url":null,"abstract":"<p>This paper offers a unique synchronization strategy for synchronizing eight chaotic systems. The new approach is referred to as dual quadratic compound anti synchronization. We additionally employed signal multi-switching to augment the complexity of the suggested technique. In communication theory, the transmission and security of the resulting signal are more effective because of the numerous combinations of chaotic systems and multiswitching that provide such complicated dynamic behavior. To demonstrate the acquired results, Lorenz, Rössler, Lü, and Chen chaotic system are used. Using the Lyapunov stability principle, sufficient conditions are attained and appropriate controllers are built to achieve the required synchronization between eight chaotic systems. To validate the findings from theory, numerical simulations, and graphics are presented using MATLAB.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"98 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2025-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142995285","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-21DOI: 10.1140/epjb/s10051-024-00857-3
M. R. Laouyenne, Mohamed Baazaoui, Fatma Aouaini, Beriham Basha, KholoudSaad Al-mugren
This research aimed to investigate the magnetic and dielectric phenomena of the La0.8Na0.2Mn0.97Fe0.03O3 sol–gel compound. Through the magnetic analysis of M (μ0H, T), we observed that the compound undergoes a ferromagnetic–paramagnetic phase transition. A perfect coincidence was observed between the magnetic entropy changes calculated using the Maxwell relation and Landau theory only in the high-temperature range. Furthermore, based on the mean field theory, we calculate the number of spins (S = 3) and the saturation magnetization (Msat = 87emu/g). With these parameters, we computed – ΔSM at different applied magnetic fields. We have observed an appreciable coincidence between -ΔSM calculated using the Maxwell relation and mean field model, confirming the validity of this technique. This suggests that the phase transition of our compound is completely described by the mean field model. Moving forward, we planned to continue investigating of the compound in our study by the critical phenomena. We calculated the critical exponent values using different approaches, such as Kouvel–Fisher, Modified Arrott plot, and critical isotherm technique. The Banerjee approach confirmed that the phase transition is of second order. We determined that the mean field model is the best description for the transition of La0.8Na0.2Mn0.97Fe0.03O3. The determined values are β = 0.43, γ = 1.09 and δ = 3.57. Finally, the total conductivity plots for the sample were established by Jonscher power law. The effect of frequency, temperature on the constant dielectric (ε") and the dielectric loss (tan δ) has been deliberated in terms of hopping of the charge carriers between Mn3+ and Mn4+ ions. Activation energy has been calculated from both temperature dependence of the continuous conductivity and the relaxation time values that confirm that same kinds of charge carriers are governing both the processes. Nyquist plot of the impedance displays semicircle arcs and the electrical equivalent circuit of the type of RG + (RGB//CPE) has been proposed to explain the impedance results.