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arXiv 1602.08692cond-mat.str-elcond-mat.otherhep-phnucl-th
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有效场论和磁振子在铁磁、反铁磁和亚铁磁中的散射过程

Effective field theory and the scattering process for magnons in the ferromagnet, antiferromagnet, and ferrimagnet

Shinya Gongyo, Yuta Kikuchi, Tetsuo Hyodo, Teiji Kunihiro

摘要:

我们讨论了依赖于SO(3)$\rightarrow$ SO(2)的低能有效拉格朗日量不仅适用于铁磁体,也适用于铁磁体和反铁磁体.对粒子态的分析表明,不仅存在色散关系为$ω\propto |\bm{k}|,\, |\bm{k}|^2$的无质量模,分别是所谓的I型和II型Nambu-Goldstone模式,而且还有与$ω\propto m^2+|\bm{k}|^2$的间隙模式。我们澄清了如何与一个时间导数和那些具有两个时间导数的有效拉格朗日项的系数确定的序参量指定是否系统是在铁磁,反铁磁或亚铁磁状态,我们强调,与自发对称性破缺的带隙模式只出现在亚铁磁系统,而不是在铁磁和反铁磁系统。我们还建立了功率计数方案,计算了两个Nambu-Goldstone玻色子之间的散射振幅和散射长度。我们证明了带隙模的散射长度是有限的,并且与带隙成正比。带隙NG模式的这一特性可用于将其与起源于其他机制的带隙激发区分开来。最后,我们研究了由外磁场和单离子各向异性给出的显式对称性破缺的影响,并表明外磁场对所有自旋系统中的散射振幅没有任何影响。相反,除了自旋为1/2的系统外,各向异性确实影响散射振幅、相移和散射长度。这一结果支持了Efimov效应在自旋系统中的可能性在以前的研究中讨论。

英文摘要:

We discuss that a low-energy effective Lagrangian relying on SO(3) $\rightarrow$ SO(2) is applicable for a ferrimagnet as well as a ferromagnet and an antiferromagnet. The analysis of the particle states shows that there exist not only massless modes with the dispersion relations $ω\propto |\bm{k}|,\, |\bm{k}|^2$, i.e., the so-called type-I and type-II Nambu-Goldstone modes, respectively, but also gapped modes with $ω\propto m^2+|\bm{k}|^2$. We clarify how the coefficients of the terms with one time derivative and those with two time derivatives in the effective Lagrangian determine the order parameters specifying whether the system is in a ferromagnetic, antiferromagnetic or ferrimagnetic state; we stress that the gapped mode related to the spontaneous symmetry breaking appears only in the ferrimagnetic system and not in the ferromagnetic and antiferromagnetic systems. We also establish the power counting scheme and calculate the scattering amplitudes and thereby the scattering lengths between the two Nambu-Goldstone bosons. We show that the scattering length of the gapped mode is finite and proportional to the gap. This characteristic property of the gapped NG mode can be used to discriminate it from gapped excitations which originate in other mechanisms. Finally, we study the effects of the explicit symmetry breaking that are given by an external magnetic field and a single-ion anisotropy, and show that the external magnetic fields do not have any effects on the scattering amplitudes in all the spin systems as was known for the ferromagnet system. In contrast, the anisotropy does affect the scattering amplitudes, the phase shift, and the scattering length except for spin 1/2 systems. This result supports the possibility of the Efimov effect in spin systems discussed in previous studies.

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