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Fractalization Drives Crystalline States In A Frustrated Spin System

机译:分形驱动沮丧的自旋系统中的晶体状态

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The fractalized Hofstadter butterfly energy spectrum predicted for magnetically confined fermions diffracted by a crystal lattice has remained beyond the reach of laboratory-accessible magnetic fields. We find the geometrically frustrated spin system SrCu_2(BO_3)_2 to provide a sterling demonstration of a system in which bosons confined by a magnetic and lattice potential mimic the behavior of fermions in the extreme quantum limit, giving rise to a sequence of plateaus at all magnetization m_z/m_(sat) = 1/q ratios 9 ≥ q ≥ 2 and p/q = 2/9 (m_(sat) is the saturation magnetization) in magnetic fields up to 85 T and temperatures down to 29 mK, within the sequence of previously identified plateaus at 1/8, 1/4, and 1/3 of the saturated magnetization. We identify this hierarchy of plateaus as a consequence of confined bosons in SrCu_2(BO_3)_2 mimicking the high magnetic field fractalization predicted by the Hofstadter butterfly for fermionic systems. Such an experimental realization of the Hofstadter problem for interacting fermions has not been previously achieved in real materials, given the unachievably high magnetic flux densities or large lattice periods required. By a theoretical treatment that includes short-range repulsion in the Hofstadter treatment, stripe-like spin density-modulated phases are revealed in SrCu_2(BO_3)_2 as emergent from a fluidic fractal spectrum.
机译:预测由晶格衍射的磁约束费米子的分形霍夫施塔特蝴蝶能谱仍然超出了实验室可达到的磁场范围。我们发现几何受挫的自旋系统SrCu_2(BO_3)_2提供了一个系统的纯正演示,在该系统中,受磁和晶格势限制的玻色子模仿了极限量子极限中费米子的行为,从而产生了一系列的平稳状态磁化强度m_z / m_(sat)= 1 / q的比率9≥q≥2且p / q = 2/9(m_(sat)是饱和磁化强度),磁场强度最高为85 T,温度最低为29 mK在饱和磁化强度的1 / 8、1 / 4和1/3处先前确定的平稳序列。我们确定了高原的这种层次结构是由于SrCu_2(BO_3)_2中的受限玻色子模仿了Hofstadter蝴蝶预测的铁磁系统的高磁场分形作用。考虑到所需的高磁通密度或大晶格周期,在实际材料中尚未实现这种与费米相互作用的霍夫施塔特问题的实验性实现。通过在Hofstadter处理中包括短程排斥的理论处理,在SrCu_2(BO_3)_2中显示出条状自旋密度调节相,这是从流体分形谱中出现的。

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