TY - JOUR
T1 - Understanding the complex metallic element Mn. II. Geometric frustration in ß-Mn, phase stability, and phase transitions
AU - Hafner, Juergen
AU - Hobbs, David
N1 - Zeitschrift: Physical Review B - Condensed Matter and Materials Physics
Coden: PRBMD
Art-Nr: 014408
Affiliations: Institut für Materialphysik, Ctr. for Compl. Materials Science, Universität Wien, Sensengasse 8/12, A-1090 Wien, Austria
Adressen: Hafner, J.; Institut für Materialphysik; Ctr. for Compl. Materials Science; Universität Wien; Sensengasse 8/12 A-1090 Wien, Austria
Import aus Scopus: 2-s2.0-0141788739
22.10.2007: Datenanforderung 1935 (Import Sachbearbeiter)
22.10.2007: Datenanforderung 1936 (Import Sachbearbeiter)
PY - 2003
Y1 - 2003
N2 - In the preceding paper [D. Hobbs, J. Hafner, and D. Spi¹ák, Phys. Rev. B 68, 014407 (2003)], we have started an ab initio spin-density-functional study of the complex structural and magnetic phase behaviors of Mn by a detailed investigation of ?-Mn. It was shown that the complex crystalline and noncollinear antiferromagnetic structures are the results of the conflicting tendencies to maximize simultaneously bond strength and magnetic moment. The present work extends this study to the remaining four polymorphs of Mn. Frustration of antiferromagnetic exchange interaction (which is the driving force leading to noncollinearity in ?-Mn) is found to be even stronger in ?-Mn. However, in contrast to the current assumption that the magnetic frustration is restricted to the sublattice of the Mn II atoms, with the Mn I atoms remaining nonmagnetic, we find that the antiferromagnetic Mn I-Mn II coupling is strongest, leading to the stabilization of a ferrimagnetic phase upon slight expansion. At equilibrium, a nonmagnetic and a weakly ferrimagnetic phase are energetically virtually degenerate. Antiferromagnetic ground states are found for ?- and ?-Mn (face- and body-centered cubic, respectively), while hexagonal ?-Mn is only marginally magnetic at equilibrium. Magnetism strongly influences the mechanical properties of all polymorphs. Due to the stabilization of the antiferromagnetic state on expansion, the ?- and ?-phase are exceptionally soft, whereas ?- and ?-Mn where magnetism is nearly completely suppressed are mechanically hard. ?-Mn is found to be soft in the noncollinear antiferromagnetic state, but hard in the nonmagnetic phase. ?-Mn is found to have the lowest energy at ambient pressure, under compression a structural phase transition to ?-Mn is predicted, in agreement with recent experiments. In summary, the structural and magnetic phase diagram of even the complex metallic element is well explained by the density-functional theory.
AB - In the preceding paper [D. Hobbs, J. Hafner, and D. Spi¹ák, Phys. Rev. B 68, 014407 (2003)], we have started an ab initio spin-density-functional study of the complex structural and magnetic phase behaviors of Mn by a detailed investigation of ?-Mn. It was shown that the complex crystalline and noncollinear antiferromagnetic structures are the results of the conflicting tendencies to maximize simultaneously bond strength and magnetic moment. The present work extends this study to the remaining four polymorphs of Mn. Frustration of antiferromagnetic exchange interaction (which is the driving force leading to noncollinearity in ?-Mn) is found to be even stronger in ?-Mn. However, in contrast to the current assumption that the magnetic frustration is restricted to the sublattice of the Mn II atoms, with the Mn I atoms remaining nonmagnetic, we find that the antiferromagnetic Mn I-Mn II coupling is strongest, leading to the stabilization of a ferrimagnetic phase upon slight expansion. At equilibrium, a nonmagnetic and a weakly ferrimagnetic phase are energetically virtually degenerate. Antiferromagnetic ground states are found for ?- and ?-Mn (face- and body-centered cubic, respectively), while hexagonal ?-Mn is only marginally magnetic at equilibrium. Magnetism strongly influences the mechanical properties of all polymorphs. Due to the stabilization of the antiferromagnetic state on expansion, the ?- and ?-phase are exceptionally soft, whereas ?- and ?-Mn where magnetism is nearly completely suppressed are mechanically hard. ?-Mn is found to be soft in the noncollinear antiferromagnetic state, but hard in the nonmagnetic phase. ?-Mn is found to have the lowest energy at ambient pressure, under compression a structural phase transition to ?-Mn is predicted, in agreement with recent experiments. In summary, the structural and magnetic phase diagram of even the complex metallic element is well explained by the density-functional theory.
U2 - 10.1103/PhysRevB.68.014408
DO - 10.1103/PhysRevB.68.014408
M3 - Article
SN - 1098-0121
VL - 68
JO - Physical Review B
JF - Physical Review B
IS - 1
M1 - 014408
ER -