论文标题

三角系统中的无质量量子自旋液体Sr $ _ {3} $ CUSB $ _ {2} $ o $ $ _ {9} $

Gapless quantum spin liquid in the triangular system Sr$_{3}$CuSb$_{2}$O$_{9}$

论文作者

Kundu, S., Shahee, Aga, Chakraborty, Atasi, Ranjith, K. M., Koo, B., Sichelschmidt, Jörg, Telling, Mark T. F., Biswas, P. K., Baenitz, M., Dasgupta, I., Pujari, Sumiran, Mahajan, A. V.

论文摘要

我们在分层三角形SR $ _ {3} $ CUSB $ _ {2} $ o $ _ {9} $(SCSO)系统中报告无质量量子旋转液体行为。 X射线衍射显示了与原子位点相关的超晶格反射,这些原子位点订购到由SB平面良好分离的三角形Cu平面。 MUON自旋放松($ $ $ sr)的测量表明,尽管有大量的curie -weiss -weiss -weiss -weiss $θ____________________________cw,$ s = \ s = \ s = \ s = \ s = \ s = \ frac {1} {1} {2} $矩仍保持动态至65 mk。从散装易感性中提取。特定的热量测量还没有显示长期订单的迹象,降低到0.35 k。在5 k下方的磁性特异性热量($ \ Mathit {C} $ _ {\ Mathrm {M}} $)5 K下方揭示了$ \ Mathit {c} $ \ mathit {c} $ _ {\ MATHRM {\ MATHRM {MATHRM {M MATHRM {M MATHRM {M MATHRM {M MATHRM {M MATHRM {M MATHRM {M MATHRM {m} $ $ = $ $ = $ $ = $ $ = $ = $ = $ $ $ $ $ ucry.显着的$ t $$^{2} $对磁性热热的贡献使现象学具有现象学,并具有线性分散体的所谓迪拉克旋转激发。从低$ t $特定的热数据中,我们估计,使用狄拉克旋转液体ansatz估计,优势交换量表为$ \ sim $ 36 K,它距离微观密度功能理论计算($ \ sim $ 45 K)的值不远,而高温易感性分析($ \ sim $ \ sim $ 70 K)。线性比热系数约为18 mJ/mol-k $^2 $,比典型的费米液体大一些。

We report gapless quantum spin liquid behavior in the layered triangular Sr$_{3}$CuSb$_{2}$O$_{9}$ (SCSO) system. X-ray diffraction shows superlattice reflections associated with atomic site ordering into triangular Cu planes well-separated by Sb planes. Muon spin relaxation ($μ$SR) measurements show that the $S = \frac{1}{2}$ moments at the magnetically active Cu sites remain dynamic down to 65 mK in spite of a large antiferromagnetic exchange scale evidenced by a large Curie-Weiss temperature $θ_{\mathrm{cw}} \simeq $ -143 K as extracted from the bulk susceptibility. Specific heat measurements also show no sign of long-range order down to 0.35 K. The magnetic specific heat ($\mathit{C}$$_{\mathrm{m}}$) below 5 K reveals a $\mathit{C}$$_{\mathrm{m}}$ $=$ $γT$ + $αT$$^{2}$ behavior. The significant $T$$^{2}$ contribution to the magnetic specific heat invites a phenomenology in terms of the so-called Dirac spinon excitations with a linear dispersion. From the low-$T$ specific heat data, we estimate the dominant exchange scale to be $\sim $ 36 K using a Dirac spin liquid ansatz which is not far from the values inferred from microscopic density functional theory calculations ($\sim $ 45 K) as well as high-temperature susceptibility analysis ($\sim$ 70 K). The linear specific heat coefficient is about 18 mJ/mol-K$^2$ which is somewhat larger than for typical Fermi liquids.

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