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On the theory of Bose-Einstein condensation of quasiparticles: On the possibility of condensation of ferromagnons at high temperatures

机译:关于准粒子的玻色-爱因斯坦凝聚理论:关于高温下铁磁子的凝聚可能性

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摘要

The Bose condensation of magnons in physical systems of finite size is considered for the case of ferromagnetic thin films. It is shown that in accordance with present-day experimental capabilities, which permit one to achieve densities of long-wavelength spin excitations of ~10{sup}18-10{sup}19 cm{sup}(-3) in such films, the formation of a coherent condensate of such quasiparticles begins at temperatures T~10{sup}2 K (including room temperature). It is found that Bose condensation is accompanied by a scaling phenomenon, according to which the main thermodynamic variable is not the number of particles N but the ratio N/T. This indicates that the Bose condensation of magnons can be observed at relatively low magnon densities (and, accordingly, low pumping). The roles played by the shape of the spectrum of spin excitations and by the film thickness for observation of the phase transition to the state with the Bose condensate are analyzed, and the partial contributions of different groups of quasiparticles to the total spectral distribution of magnons over energies are discussed.
机译:对于铁磁薄膜,考虑在有限尺寸的物理系统中磁振子的玻色凝聚。结果表明,根据当今的实验能力,可以使这样的薄膜达到〜10 {sup} 18-10 {sup} 19 cm {sup}(-3)的长波长自旋激发的密度,这种准粒子的凝聚凝结物的形成始于温度T〜10 {sup} 2 K(包括室温)。已经发现,玻色冷凝伴随着结垢现象,据此,主要的热力学变量不是颗粒数目N而是比率N / T。这表明可以在相对较低的马农密度下观察到马农的玻色凝结(因此,泵浦度较低)。分析了自旋激发光谱的形状和膜厚对观察玻色子凝结到状态的转变所起的作用,并分析了不同组准粒子对磁振子总谱分布的部分贡献。讨论能量。

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