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Developing the Pressure-Temperature-Magnetic Field Phase Diagram of Multiferroic [(CH3)2NH2]Mn(HCOO)3.
Clune, Amanda; Harms, Nathan; O'Neal, Kenneth R; Hughey, Kendall; Smith, Kevin A; Obeysekera, Dimuthu; Haddock, John; Dalal, Naresh S; Yang, Junjie; Liu, Zhenxian; Musfeldt, Janice L.
Afiliação
  • Clune A; Department of Chemistry, University of Tennessee, Knoxville, Tennessee 37996, United States.
  • Harms N; Department of Chemistry, University of Tennessee, Knoxville, Tennessee 37996, United States.
  • O'Neal KR; Department of Chemistry, University of Tennessee, Knoxville, Tennessee 37996, United States.
  • Hughey K; Department of Chemistry, University of Tennessee, Knoxville, Tennessee 37996, United States.
  • Smith KA; Department of Chemistry, University of Tennessee, Knoxville, Tennessee 37996, United States.
  • Obeysekera D; Department of Physics, Central Michigan University, Mount Pleasant, Michigan 48859, United States.
  • Haddock J; Department of Physics, New Jersey Institute of Technology, Newark, New Jersey 07102, United States.
  • Dalal NS; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, United States.
  • Yang J; National High Magnetic Field Laboratory, Tallahassee, Florida 32310, United States.
  • Liu Z; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, United States.
  • Musfeldt JL; National High Magnetic Field Laboratory, Tallahassee, Florida 32310, United States.
Inorg Chem ; 59(14): 10083-10090, 2020 Jul 20.
Article em En | MEDLINE | ID: mdl-32635719
ABSTRACT
We combined Raman scattering and magnetic susceptibility to explore the properties of [(CH3)2NH2]Mn(HCOO)3 under compression. Analysis of the formate bending mode reveals a broad two-phase region surrounding the 4.2 GPa critical pressure that becomes increasingly sluggish below the order-disorder transition due to the extensive hydrogen-bonding network. Although the paraelectric and ferroelectric phases have different space groups at ambient-pressure conditions, they both drive toward P1 symmetry under compression. This is a direct consequence of how the order-disorder transition changes under pressure. We bring these findings together with prior magnetization work to create a pressure-temperature-magnetic field phase diagram, unveiling entanglement, competition, and a progression of symmetry-breaking effects that underlie functionality in this molecule-based multiferroic. That the high-pressure P1 phase is a subgroup of the ferroelectric Cc suggests the possibility of enhanced electric polarization as well as opportunity for strain control.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2020 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2020 Tipo de documento: Article