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Spontaneous decays of magneto-elastic excitations in non-collinear antiferromagnet (YLu)MnO3

机译:非共线反铁磁体(YLu)MnO3中磁弹性激发的自发衰减

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摘要

Magnons and phonons are fundamental quasiparticles in a solid and can be coupled together to form a hybrid quasi-particle. However, detailed experimental studies on the underlying Hamiltonian of this particle are rare for actual materials. Moreover, the anharmonicity of such magnetoelastic excitations remains largely unexplored, although it is essential for a proper understanding of their diverse thermodynamic behaviour and intrinsic zero-temperature decay. Here we show that in non-collinear antiferromagnets, a strong magnon–phonon coupling can significantly enhance the anharmonicity, resulting in the creation of magnetoelastic excitations and their spontaneous decay. By measuring the spin waves over the full Brillouin zone and carrying out anharmonic spin wave calculations using a Hamiltonian with an explicit magnon–phonon coupling, we have identified a hybrid magnetoelastic mode in (Y,Lu)MnO3 and quantified its decay rate and the exchange-striction coupling term required to produce it.
机译:磁振子和声子是固体中的基本准粒子,可以耦合在一起形成杂化准粒子。但是,对于实际材料,很少有关于该粒子潜在的哈密顿量的详细实验研究。此外,尽管对于正确理解它们的各种热力学行为和固有的零温度衰减是必不可少的,但这种磁弹性激发的非谐性仍未得到充分探索。在这里,我们表明,在非共线反铁磁体中,强磁子-声子耦合可以显着增强非谐性,从而导致磁弹性激发的产生及其自发衰减。通过测量整个布里渊区的自旋波并使用具有显式磁振子-声子耦合的哈密顿量进行非谐自旋波计算,我们确定了(Y,Lu)MnO3的混合磁弹性模式并量化了其衰减率和交换产生它的-收缩耦合项。

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