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The flux dynamics behavior of the two competing high temperature superconducting phases in underdoped LaCuO$_{4.06}$

机译:掺杂不足的LaCuO中两个竞争的高温超导相的通量动力学行为__ {4.06} $

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摘要

In complex transition metal oxides (TMO) an arrested electronic phase separation (PS) appears by tuning the system near a Lifshitz transition in multiband Hubbard models. The PS in La$_2$CuO$_{4+y}$ near insulator to metal transition (IMT) is made of short range Charge Density Wave (CDW) order inhomogeneity coexisting with quenched lattice disorder. While at high doping y = 0.1 percolation gives a single superconducting phase, near the IMT at y = 0.06 two coexisting superconducting phases appear: the first one with a critical temperature T$_{c1}$ = 16 K and the second one with T$_{c2}$ = 29 K. It is known that the two superconducting phases are characterized by two different space geometry because of two different spatial distributions of both CDW order and dopants self-organization. Here we show that these two phases show different flux dynamic regimes using alternating current (AC) multi-harmonic susceptibility experiments. This is a unique technique capable to investigate multi-phase superconductors and characterize their transport properties in a percolative scenario. Results point out that the low critical temperature phase is well described by a bulk-like flux pinning with a 2D geometry while the phase with higher critical temperature shows a ‘barrier pinning’ mechanism providing direct evidence of two different superconducting vortex dynamics in different complex geometrical spaces.
机译:在复杂过渡金属氧化物(TMO)中,通过在多频带Hubbard模型中的Lifshitz跃迁附近调整系统,会出现停滞的电子相分离(PS)。 La $ _2 $ CuO $ _ {4 + y} $接近绝缘子到金属的转变(IMT)中的PS由短距离电荷密度波(CDW)阶不均匀性与淬灭晶格无序共存而成。在高掺杂y = 0.1时,渗流会产生一个超导相,在y = 0.06的IMT附近,出现两个共存的超导相:第一个临界温度为T $ _ {c1} $ = 16 K,第二个为T $ _ {c2} $ = 29K。众所周知,这两个超导相的特征在于两个不同的空间几何形状,这是由于CDW阶和掺杂剂自组织的两个不同的空间分布。在这里,我们显示这两个阶段使用交流(AC)多谐波磁化率实验显示了不同的通量动态范围。这是一种独特的技术,能够研究多相超导体并在渗流情况下表征其传输特性。结果指出,低临界温度相通过具有二维几何形状的块状通量钉扎得到了很好的描述,而临界温度较高的相表现出“势垒钉扎”机制,提供了在不同复杂几何形状中两种不同超导涡旋动力学的直接证据。空格。

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