TY - JOUR
T1 - Inelastic neutron scattering study on anisotropic exchange and dzyaloshinsky–moriya interactions in the S= 1/2 Triangular Spin Cluster V3
AU - Iida, Kazuki
AU - Sato, Taku J.
AU - Yamase, Toshihiro
N1 - Funding Information:
The work was supported by a Grant-in-Aid for Scientific Research (17002006) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT). One (K.I.) of us acknowledges the support from the Global COE Program ‘‘the Physical Sciences Frontier’’, MEXT. We would like to thank N. Aso, T. Asami, and Y. Kawamura for their help in our INS experiments.
Publisher Copyright:
© 2009 The Physical Society of Japan
PY - 2009/11
Y1 - 2009/11
N2 - Inelastic neutron scattering (INS) experiments have been performed on a V3 triangular spin cluster. At the base temperature (T = 0:7 K), the INS spectrum clearly exhibits a broad peak at h ! = 0:8 meV. The peak was ascribed to the superposition of four magnetic excitations from two Stotal = 1=2 doublets to two Stotal = 3=2 doublets. From the observed peak position, width, and intensity, we confirmed a model Hamiltonian comprising anisotropic exchange and Dzyaloshinsky–Moriya (DM) interactions, and estimated the Hamiltonian parameters as Jx = Jy = 5:73 K, Jz = 6:83 K, Dz1;2 = 0:261 K, and Dz2;3 = Dz3;1 = 0:287 K, where J is the -component of the exchange interactions and Dzi; j represents the z-component of the DM vector between the i-th and j-th V4þ ions. The resulting model Hamiltonian successfully reproduced the half-step magnetization process reported earlier as well as magnetic susceptibility.
AB - Inelastic neutron scattering (INS) experiments have been performed on a V3 triangular spin cluster. At the base temperature (T = 0:7 K), the INS spectrum clearly exhibits a broad peak at h ! = 0:8 meV. The peak was ascribed to the superposition of four magnetic excitations from two Stotal = 1=2 doublets to two Stotal = 3=2 doublets. From the observed peak position, width, and intensity, we confirmed a model Hamiltonian comprising anisotropic exchange and Dzyaloshinsky–Moriya (DM) interactions, and estimated the Hamiltonian parameters as Jx = Jy = 5:73 K, Jz = 6:83 K, Dz1;2 = 0:261 K, and Dz2;3 = Dz3;1 = 0:287 K, where J is the -component of the exchange interactions and Dzi; j represents the z-component of the DM vector between the i-th and j-th V4þ ions. The resulting model Hamiltonian successfully reproduced the half-step magnetization process reported earlier as well as magnetic susceptibility.
KW - Dzyaloshinsky–Moriya
KW - Inelastic neutron scattering
KW - Molecular nanomagnet
KW - Spin trimer system
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U2 - 10.1143/JPSJ.78.114709
DO - 10.1143/JPSJ.78.114709
M3 - Article
AN - SCOPUS:80052382876
SN - 0031-9015
VL - 78
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 11
M1 - 114709
ER -