热输运对低频顺磁自旋-晶格弛豫实验的影响

J. Flokstra, G.J. Gerritsma, G.A. Hartemink, L.C. Van Der Marel
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引用次数: 14

摘要

在放置在液氦中的顺磁晶体的低频弛豫实验中,经常发现色散和吸收曲线与卡西米尔和杜·普莱尔的热力学理论大相径庭。对于与吸收曲线最大值有关的弛豫时间τabs, τabs αT-α与1 <呈温度依赖性;α& lt;6经常被发现,有时伴随着氦转变温度Tλ的跳跃。我们从包含晶格和氦浴的热传导以及晶体到浴的热阻的模型出发,计算了色散和吸收曲线,发现假设自旋-晶格弛豫的直接过程,τabs(T)(与计算的吸收曲线的最大值相关)可以大致如上所述,在Tγ处有一个跳跃。
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On the influence of heat transport on low- frequency paramagnetic spin—Lattice relaxation experiments

In low-frequency relaxation experiments on paramagnetic crystals, placed in liquid helium, often dispersion- and absorption curves are found, strongly deviating from those following from the thermodynamic theory of Casimir and Du Pré. For the relaxation time τabs, related to the maximum in the absorption curve, a temperature dependence τabs αT with 1 < α < 6 has been found frequently, accompanied sometimes with a jump at the helium-transition temperature Tλ. We computed, starting from a model including the heat conduction of lattice and helium bath and a heat resistance from crystal to bath, dispersion- and absorption curves and found that, assuming the direct process for the spin—lattice relaxation, τabs(T) (related to the maximum of the calculated absorption curve) can be described roughly as mentioned above with a jump at Tγ.

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