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Duality in 2+1D Quantum Elasticity: superconductivity and Quantum Nematic Order

机译:2 + 1D量子弹性的对偶性:超导性和量子   向列秩序

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摘要

The generalization of the Nelson-Halperin-Young theory of 2D melting to thedynamical 2+1D quantum case is presented. The bosonic quantum crystal dualizesin superfluids or superconductors exhibiting nematic liquid crystalline orders,corresponding with bose condensates of dislocations exhibiting a dual shearMeissner-Higgs mechanism. The topologically ordered nematic phase suggested byLammert, Toner and Rokshar finds a simple interpretation in this framework. Theordered nematic is a true quantum phase: the dynamical glide principleinterferes with the effect that the phonon spectrum of the crystal re-emergesin the direction orthogonal to the director. Novel insights follow from theduality on the fundamental nature of superfluidity and superconductivity. Thesuperfluid can be viewed as an elastic medium having lost its rigidity againstshear stresses. Upon dualizing the electrically charged crystal theelectromagnetic Meissner phase is recovered, showing peculiar screening currentoscillations when the shear penetration depth becomes larger than the Londonpenetration depth.
机译:提出了Nelson-Halperin-Young的2D熔化理论到动态2 + 1D量子情况的推广。呈现出向列型液晶顺序的玻色子量子二元体超流体或超导体,与位错的玻色凝结相应,表现出双剪切Meissner-Higgs机理。 Lammert,Toner和Rokshar建议的拓扑有序向列相可以在此框架中找到简单的解释。有序的向列是真正的量子相:动态滑移原理会干扰晶体的声子谱在正交于指向矢的方向上重新出现。从对偶性的角度出发,对超流体和超导电性的基本本质有了新的见解。可以将超流体视为一种抗剪切应力而失去刚性的弹性介质。在使带电的晶体双重化之后,电磁的迈斯纳相被恢复,当剪切穿透深度变得大于伦敦穿透深度时,显示出独特的屏蔽电流振荡。

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