TY - JOUR
T1 - Magnetic structures and excitations in a multiferroic Y-type hexaferrite BaSrCo2Fe11AlO22
AU - Nakajima, Taro
AU - Tokunaga, Yusuke
AU - Matsuda, Masaaki
AU - Dissanayake, Sachith
AU - Fernandez-Baca, Jaime
AU - Kakurai, Kazuhisa
AU - Taguchi, Yasujiro
AU - Tokura, Yoshinori
AU - Arima, Taka Hisa
N1 - Publisher Copyright:
© 2016 American Physical Society.
PY - 2016
Y1 - 2016
N2 - We have investigated magnetic orders and excitations in a Y-type hexaferrite BaSrCo2Fe11AlO22 (BSCoFAO), which was reported to exhibit spin-driven ferroelectricity at room temperature [S. Hirose, K. Haruki, A. Ando, and T. Kimura, Appl. Phys. Lett. 104, 022907 (2014)10.1063/1.4862432]. By means of magnetization, electric polarization, and neutron-diffraction measurements using single-crystal samples, we establish a H-T magnetic phase diagram for magnetic field perpendicular to the c axis (H?c). This system exhibits an alternating longitudinal conical (ALC) magnetic structure in the ground state, and it turns into a non-co-planar commensurate magnetic order with spin-driven ferroelectricity under H?c. The field-induced ferroelectric phase remains as a metastable state after removing magnetic field below ∼250 K. This metastability is the key to understanding of magnetic field reversal of the spin-driven electric polarization in this system. Inelastic polarized neutron-scattering measurements in the ALC phase reveal a magnetic excitation at around 7.5 meV, which is attributed to spin components oscillating in a plane perpendicular to the cone axis. This phasonlike excitation is expected to be an electric-field active magnon, i.e., electromagnon excitation, in terms of the magnetostriction mechanism.
AB - We have investigated magnetic orders and excitations in a Y-type hexaferrite BaSrCo2Fe11AlO22 (BSCoFAO), which was reported to exhibit spin-driven ferroelectricity at room temperature [S. Hirose, K. Haruki, A. Ando, and T. Kimura, Appl. Phys. Lett. 104, 022907 (2014)10.1063/1.4862432]. By means of magnetization, electric polarization, and neutron-diffraction measurements using single-crystal samples, we establish a H-T magnetic phase diagram for magnetic field perpendicular to the c axis (H?c). This system exhibits an alternating longitudinal conical (ALC) magnetic structure in the ground state, and it turns into a non-co-planar commensurate magnetic order with spin-driven ferroelectricity under H?c. The field-induced ferroelectric phase remains as a metastable state after removing magnetic field below ∼250 K. This metastability is the key to understanding of magnetic field reversal of the spin-driven electric polarization in this system. Inelastic polarized neutron-scattering measurements in the ALC phase reveal a magnetic excitation at around 7.5 meV, which is attributed to spin components oscillating in a plane perpendicular to the cone axis. This phasonlike excitation is expected to be an electric-field active magnon, i.e., electromagnon excitation, in terms of the magnetostriction mechanism.
UR - http://www.scopus.com/inward/record.url?scp=85000501087&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.94.195154
DO - 10.1103/PhysRevB.94.195154
M3 - Article
AN - SCOPUS:85000501087
SN - 2469-9950
VL - 94
JO - Physical Review B
JF - Physical Review B
IS - 19
M1 - 195154
ER -