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Equilibrium low temperature heat capacity of the spin density wave compound (TMTTF)_2Br: effect of a magnetic field

机译:自旋密度波化合物(TMTTF)_2Br的平衡低温热容:磁场的影响

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We have investigated the effect of the magnetic field (B) on the very low-temperature equilibrium heat capacity ceq of the quasi-1 D organic compound (TMTTF)2Br, characterized by a commensurate Spin Density Wave (SDW) ground state. Below 1 K, ceq is dominated by a Schottky-like AST-2 contribution, very sensitive to the experimental time scale, a property that we have previously measured in numerous DW compounds. Under applied field (in the range 0.2–7 T), the equilibrium dynamics, and hence ceq extracted from the time constant, increases enormously. For B 2–3 T, ceq varies like B2, in agreement with a magnetic Zeeman coupling. Another specific property, common to other Charge/Spin density wave (DW) compounds, is the occurrence of metastable branches in ceq, induced at very low temperature by the field exceeding a critical value. These effects are discussed within a generalization to SDWs in a magnetic field of the available Larkin-Ovchinnikov local model of strong pinning. A limitation of the model when compared to experiments is pointed out.
机译:我们已经研究了磁场(B)对准1 D有机化合物(TMTTF)2Br的非常低温平衡热容ceq的影响,其特征是相应的自旋密度波(SDW)基态。低于1 K时,ceq主要由类似于肖特基的AST-2贡献所决定,它对实验时间尺度非常敏感,这是我们之前在众多DW化合物中测得的特性。在外加磁场(0.2-7 T范围内)下,平衡动力学以及从时间常数中提取的ceq大大增加。对于B 2–3 T,与磁塞曼耦合一致,ceq像B2一样变化。其他电荷/自旋密度波(DW)化合物共有的另一个特定属性是ceq中亚稳分支的出现,该电场在很低的温度下由超过临界值的电场引起。在对强钉扎可用的Larkin-Ovchinnikov局部模型的磁场中的SDW的概括中,讨论了这些影响。指出了与实验相比模型的局限性。

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