Effect of the Magnetic Field on the des Cloizeaux-Pearson Spin-Wave Spectrum
Effect of the Magnetic Field on the des Cloizeaux-Pearson Spin-Wave Spectrum
复制标题
磁场对 Cloizeaux-Pearson 自旋波谱的影响
DOI:
10.1143/ptp.57.1862
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发表时间:
1977
影响因子:
--
通讯作者:
H. Shiba
中科院分区:
文献类型:
--
作者:
N. Ishimura;H. Shiba
The des Cloizeaux and Pearson's exact solution for the spin-wave spectrum of the S=1/2 antiferromagnetic Heisenberg chain is extended to the case of finite external field. It reproduces naturally the des Cloizeaux-Pearson spectrum in the zero-field limit as well as the spin-wave spectrum in the ferromagnetic state for fields larger than the critical field. The results are discussed by comparing them with predictions of other approximate theories. on CuC12 • 2NC,D,, which is a typical 1D antiferromagnetic Heisenberg spin system with S = 1/2. They showed by neutron scattering that its spin-wave spectrum agrees quite well with the celebrated exact solution of des Cloizeaux and Pearson ( dC-P) ;l and is in disagreement with the Anderson (molecular-field) theory. It clearly demonstrates the importance of exact theoretical studies of 1D systems. Although this experiment was made in the absence of external magnetic field, the magnetic-field dependence of elementary excitations in antiferromagnetic linear chains would be very interesting. The purpose of this paper is to study exactly the magnetic-field dependence of the dC-P spin-wave spectrum. We hope that this work would stimulate further experimental studies on dynamics of 1D Heisenberg antiferromagnets in the presence of external field. The field dependence of spin waves of lD Heisenberg antifer romagnets has previously been calculated by Pytte,"l who applied the Bulaevskii (Hartree-Fock) approximation') based on the Fermion representation 5l.Bl of the lD Heisenberg model. We later compare it with our result. We also show that the magnetic-field dependence of the dC-P spin wave is qualitatively different from that of the classical (Anderson) spin wave. The details of the formulation and calculations are presented in § 2. Com-