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Structure-Property Relationships in α-, ß'-, and γ-Modifications of Mn3(PO4)2.
Volkova, Olga S; Shvanskaya, Larisa V; Ovchenkov, Evgeny A; Zvereva, Elena A; Volkov, Anatoly S; Chareev, Dmitriy A; Molla, Kaimujjaman; Rahaman, Badiur; Saha-Dasgupta, Tanusri; Vasiliev, Alexander N.
Afiliação
  • Volkova OS; M. V. Lomonosov Moscow State University , Moscow 119991, Russia.
  • Shvanskaya LV; National University of Science and Technology , Moscow 119049, Russia.
  • Ovchenkov EA; Ural Federal University , Ekaterinburg 620002, Russia.
  • Zvereva EA; M. V. Lomonosov Moscow State University , Moscow 119991, Russia.
  • Volkov AS; National University of Science and Technology , Moscow 119049, Russia.
  • Chareev DA; M. V. Lomonosov Moscow State University , Moscow 119991, Russia.
  • Molla K; M. V. Lomonosov Moscow State University , Moscow 119991, Russia.
  • Rahaman B; M. V. Lomonosov Moscow State University , Moscow 119991, Russia.
  • Saha-Dasgupta T; Ural Federal University , Ekaterinburg 620002, Russia.
  • Vasiliev AN; Institute of Experimental Mineralogy, RAS , Chernogolovka 142432, Russia.
Inorg Chem ; 55(20): 10692-10700, 2016 Oct 17.
Article em En | MEDLINE | ID: mdl-27661209
The manganese orthophosphate, Mn3(PO4)2, is characterized by the rich variety of polymorphous modifications, α-, ß'-, and γ-phases, crystallized in monoclinic P21/c (P21/n) space group type with unit cell volume ratios of 2:6:1. The crystal structures of these phases are constituted by three-dimensional framework of corner- and edge-sharing [MnO5] and [MnO6] polyhedra strengthened by [PO4] tetrahedra. All compounds experience long-range antiferromagnetic order at Neel temperature TN = 21.9 K (α-phase), 12.3 K (ß'-phase), and 13.3 K (γ-phase). Additionally, second magnetic phase transition takes place at T* = 10.3 K in ß'-phase. The magnetization curves of α- and ß'-modifications evidence spin-floplike features at B = 1.9 and 3.7 T, while the γ-Mn3(PO4)2 stands out for an extended one-third magnetization plateau stabilized in the range of magnetic field B = 7.5-23.5 T. The first-principles calculations define the main paths of superexchange interaction between Mn spins in these polymorphs. The spin model for α-phase is found to be characterized by collection of uniform and alternating chains, which are coupled in all three directions. The strongest magnetic exchange interaction in γ-phase emphasizes the trimer units, which make chains that are in turn weakly coupled to each other. The spin model of ß'-phase turns out to be more complex compared to α- or γ-phase. It shows complex chain structures involving exchange interactions between Mn2 (Mn2', Mn2″) and Mn3 (Mn3', Mn3″). These chains interact through exchanges involving Mn1 (Mn1', Mn1″) spins.
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Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Inorg Chem Ano de publicação: 2016 Tipo de documento: Article País de afiliação: Federação Russa
Buscar no Google
Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Inorg Chem Ano de publicação: 2016 Tipo de documento: Article País de afiliação: Federação Russa