Tomonaga-Luttinger liquid and quantum criticality in spin-½ antiferromagnetic Heisenberg chain C14H18CuN4O10 via Wilson ratio

Sharath Kumar Channarayappa, Sankalp Kumar, N S Vidhyadhiraja, Sumiran Pujari, M P Saravanan, Amal Sebastian, Eun Sang Choi, Shalinee Chikara, Dolly Nambi, Athira Suresh, Siddhartha Lal, D Jaiswal-Nagar
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Abstract

The ground state of a one-dimensional spin-½ uniform antiferromagnetic Heisenberg chain (AfHc) is a Tomonaga-Luttinger liquid which is quantum-critical with respect to applied magnetic fields upto a saturation field μ0 Hs beyond which it transforms to a fully polarised state. Wilson ratio has been predicted to be a good indicator for demarcating these phases [Phys. Rev. B 96, 220401 (2017)]. From detailed temperature and magnetic field dependent magnetisation, magnetic susceptibility and specific heat measurements in a metalorganic complex and comparisons with field theory and quantum transfer matrix method calculations, the complex was found to be a very good realisation of a spin-½ AfHc. Wilson ratio obtained from experimentally obtained magnetic susceptibility and magnetic contribution of specific heat values was used to map the magnetic phase diagram of the uniform spin-½ AfHc over large regions of phase space demarcating Tomonaga-Luttinger liquid, saturation field quantum critical, and fully polarised states. Luttinger parameter and spinon velocity were found to match very well with the values predicted from conformal field theory.
自旋½反铁磁性海森堡链 C14H18CuN4O10 中通过威尔逊比的 Tomonaga-Luttinger 液体和量子临界性
一维自旋½均匀反铁磁性海森堡链(AfHc)的基态是一种友永-鲁丁格液体,相对于外加磁场而言,它是量子临界的,直到饱和磁场μ0 Hs为止,超过饱和磁场,它就会转变为完全极化态。据预测,威尔逊比是划分这些相的良好指标[Phys. Rev. B 96, 220401 (2017)]。通过对金属有机复合物进行详细的温度和磁场相关磁化、磁感应强度和比热测量,并与场论和量子传递矩阵法计算进行比较,发现该复合物是自旋½ AfHc 的很好实现。利用从实验中获得的磁感应强度和磁贡献比热值得出的威尔逊比值,绘制出了均匀自旋½ AfHc 的磁相图,该磁相图覆盖了划分为 Tomonaga-Luttinger 液体、饱和场量子临界和完全极化态的大面积相空间。研究发现,卢廷格参数和自旋子速度与共形场理论预测的值非常吻合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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