Calculation of the Magnetization and the Heat Capacity for [Nh2 Nh3][M(hcoo)3] (M=fe, Mn) Near the Phase Transitions
dc.authorscopusid | 9334413200 | |
dc.authorscopusid | 57990730000 | |
dc.authorwosid | Yurtseven, Hasan/Aba-9994-2020 | |
dc.contributor.author | Yurtseven, H. | |
dc.contributor.author | Dogan, E. Kilit | |
dc.date.accessioned | 2025-05-10T17:20:57Z | |
dc.date.available | 2025-05-10T17:20:57Z | |
dc.date.issued | 2022 | |
dc.department | T.C. Van Yüzüncü Yıl Üniversitesi | en_US |
dc.department-temp | [Yurtseven, H.] Middle East Tech Univ, Dept Phys, Ankara, Turkey; [Dogan, E. Kilit] Yuzuncu Yil Univ, Dept Phys, Van, Turkey | en_US |
dc.description.abstract | Temperature dependence of the magnetization M(T) is calculated for [NH2 NH3][M(HCOO)(3)] (M=Fe, Mn), namely, HyFe (perovskite and chiral) below T m =12.5 K and, for HyMn (chiral) below and above T m =7.9 K (at 100 Oe) by the molecular field theory (MFT). Close to the magnetic transition temperature ( T m ), the temperature (at 100 Oe) and the field (at 2K) dependence of the magnetization M(T, H) is analyzed by the power-law formula using the literature data. Magnetic susceptibility is predicted as a function of the field (T = 2K). Also, the temperature dependence of the heat capacity is calculated by the compressible Ising model close to the structural phase transitions in perovskite ( T C =347 K) and chiral ( T C =336 K) HyFe and the chiral ( T C =296 K) HyMn. Our results indicate that HyM (M=Fe, Mn) exhibit weak first order or near second order transitions (magnetic transition and the structural phase transitions). | en_US |
dc.description.woscitationindex | Science Citation Index Expanded | |
dc.identifier.doi | 10.1080/00150193.2022.2115799 | |
dc.identifier.endpage | 87 | en_US |
dc.identifier.issn | 0015-0193 | |
dc.identifier.issn | 1563-5112 | |
dc.identifier.issue | 1 | en_US |
dc.identifier.scopus | 2-s2.0-85143197606 | |
dc.identifier.scopusquality | Q4 | |
dc.identifier.startpage | 73 | en_US |
dc.identifier.uri | https://doi.org/10.1080/00150193.2022.2115799 | |
dc.identifier.uri | https://hdl.handle.net/20.500.14720/10260 | |
dc.identifier.volume | 600 | en_US |
dc.identifier.wos | WOS:000894426900007 | |
dc.identifier.wosquality | Q4 | |
dc.language.iso | en | en_US |
dc.publisher | Taylor & Francis Ltd | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Magnetization M(T | en_US |
dc.subject | H) | en_US |
dc.subject | Heat Capacity Cp(T) | en_US |
dc.subject | Molecular Field Theory | en_US |
dc.subject | An Ising Model | en_US |
dc.subject | Power-Law Analysis | en_US |
dc.subject | Hym (M=Fe | en_US |
dc.subject | Mn) | en_US |
dc.title | Calculation of the Magnetization and the Heat Capacity for [Nh2 Nh3][M(hcoo)3] (M=fe, Mn) Near the Phase Transitions | en_US |
dc.type | Article | en_US |