The study of structural, electronic, magnetic and magnetocaloric properties of antiperovskite carbides M3AlC (M=Mn and Fe): DFT combined with Monte Carlo simulation
A. Azouaoui, S. Mouchou, Y. Toual, N. Benzakour, A. Hourmatallah
{"title":"The study of structural, electronic, magnetic and magnetocaloric properties of antiperovskite carbides M3AlC (M=Mn and Fe): DFT combined with Monte Carlo simulation","authors":"A. Azouaoui, S. Mouchou, Y. Toual, N. Benzakour, A. Hourmatallah","doi":"10.1142/s0217984924502816","DOIUrl":null,"url":null,"abstract":"<p>This work aims to investigate the structural stability, magnetic and electronic properties of M<sub>3</sub>AlC antiperovskites using density functional theory (DFT) and Monte Carlo simulation. The obtained ground state results reveal that the antiperovskites M<sub>3</sub>AlC are stable in the ferromagnetic (FM) state with a metallic character. The calculated total magnetic moments are 5.21<span><math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>μ</mi></mrow><mrow><mi>B</mi></mrow></msub></math></span><span></span> and 3.34<span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>μ</mi></mrow><mrow><mi>B</mi></mrow></msub></math></span><span></span> for Mn<sub>3</sub>AlC and Fe<sub>3</sub>AlC, respectively, with the total moments mainly from the M atom. The ferromagnetic behavior is confirmed by computing the density of state at Fermi level and verified the Stoner criterion. The magnetic and magnetocaloric behavior of M<sub>3</sub>AlC is investigated using Monte Carlo simulation and the obtained results demonstrate that the transition from ferromagnetic to paramagnetic state occurs at <span><math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>T</mi></mrow><mrow><mi>C</mi></mrow></msub><mo>=</mo><mn>3</mn><mn>0</mn><mn>0</mn></math></span><span></span><span><math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>K and <span><math altimg=\"eq-00006.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>T</mi></mrow><mrow><mi>C</mi></mrow></msub><mo>=</mo><mn>2</mn><mn>3</mn><mn>0</mn></math></span><span></span><span><math altimg=\"eq-00007.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>K for Mn<sub>3</sub>AlC and Fe<sub>3</sub>AlC, respectively. These values of <span><math altimg=\"eq-00008.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>T</mi></mrow><mrow><mi>C</mi></mrow></msub></math></span><span></span> are in good agreement with the experimental results. The magnetocaloric effect and critical behavior are studied and the obtained values of magnetic entropy change <span><math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"><mi>|</mi><mi mathvariant=\"normal\">Δ</mi><msub><mrow><mi>S</mi></mrow><mrow><mstyle><mtext mathvariant=\"normal\">mag</mtext></mstyle></mrow></msub><mi>|</mi></math></span><span></span> at 4.5<span><math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>T is about 4.242<span><math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>J/kg.K and 3.666<span><math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>J/kg.K and the relative cooling power (RCP) are 342.434<span><math altimg=\"eq-00013.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>J/kg.K and 325.26<span><math altimg=\"eq-00014.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>J/kg.K for Mn<sub>3</sub>AlC and Fe<sub>3</sub>AlC at 4.5T, indicating that these compounds are more appropriate for magnetic refrigeration. Finally, the critical exponents (<span><math altimg=\"eq-00015.gif\" display=\"inline\" overflow=\"scroll\"><mi>β</mi></math></span><span></span>,<span><math altimg=\"eq-00016.gif\" display=\"inline\" overflow=\"scroll\"><mi>γ</mi></math></span><span></span>,<span><math altimg=\"eq-00017.gif\" display=\"inline\" overflow=\"scroll\"><mi>δ</mi></math></span><span></span>) are calculated and the obtained values are close to the values of mean-field model.</p>","PeriodicalId":18570,"journal":{"name":"Modern Physics Letters B","volume":"86 1","pages":""},"PeriodicalIF":1.8000,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Modern Physics Letters B","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1142/s0217984924502816","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, APPLIED","Score":null,"Total":0}
引用次数: 0
Abstract
This work aims to investigate the structural stability, magnetic and electronic properties of M3AlC antiperovskites using density functional theory (DFT) and Monte Carlo simulation. The obtained ground state results reveal that the antiperovskites M3AlC are stable in the ferromagnetic (FM) state with a metallic character. The calculated total magnetic moments are 5.21 and 3.34 for Mn3AlC and Fe3AlC, respectively, with the total moments mainly from the M atom. The ferromagnetic behavior is confirmed by computing the density of state at Fermi level and verified the Stoner criterion. The magnetic and magnetocaloric behavior of M3AlC is investigated using Monte Carlo simulation and the obtained results demonstrate that the transition from ferromagnetic to paramagnetic state occurs at K and K for Mn3AlC and Fe3AlC, respectively. These values of are in good agreement with the experimental results. The magnetocaloric effect and critical behavior are studied and the obtained values of magnetic entropy change at 4.5T is about 4.242J/kg.K and 3.666J/kg.K and the relative cooling power (RCP) are 342.434J/kg.K and 325.26J/kg.K for Mn3AlC and Fe3AlC at 4.5T, indicating that these compounds are more appropriate for magnetic refrigeration. Finally, the critical exponents (,,) are calculated and the obtained values are close to the values of mean-field model.
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