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Anyon Bosonization of 2D Fermions and Single Boson Phase Diagram Implied from Experiment on Visualizing Pair Formation in Superconductor Bi_2Sr_2CaCu_2O_{8+\delta}

机译:暗示了2D费米子和单个玻色子相图的任意玻色化   可视化超导体中对的形成实验   Bi_2sr_2CaCu_2O_ {8+ \增量}

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摘要

Recently, Gomes et al. [1] have visualized the gap formation in nanoscaleregions (NRs) above the critical temperature T_c in the high-T_c superconductorBi_2Sr_2CaCu_2O_{8+\delta}. It has been found that, as the temperature lowers,the NRs expand in the bulk superconducting state consisted of inhomogeneities.The fact that the size of the inhomogeneity [2] is close to the minimal size ofthe NR [1] leads to a conclusion that the superconducting phase is a result ofthese overlapped NRs. In the present paper we perform the charge andpercolation regime analysis of NRs and show that at the first critical dopingx_{c1}, when the superconductivity starts on, each NR carries the positiveelectric charge one in units of electron charge, thus we attribute the NR to asingle hole boson, and the percolation lines connecting these bosons emerge. Atthe second critical doping x_{c2}, when the superconductivity disappears, ouranalysis demonstrates that the charge of each NR equals two. The origin ofx_{c2} can be understood by introducing additional normal phase hole fermionsin NRs, whose concentration appearing above x_{c1} increases smoothly with thedoping and breaks the percolation lines of bosons at x_{c2}. The last oneresults in disappearing the bulk bosonic property of the pseudogap (PG) region,which explains the upper bound for existence of vortices in Nernst effect [3].Since [1] has demonstrated the absence of NRs at the PG boundary one canconclude that along this boundary, as well as in x_{c2}, all bosons disappear.As justification of appearance of single bosons, the bosonization of 2Dfermions is rigorously proven using the concept of anyons. The linear densitydependence of the energy gap between excited fermionic and bosonic groundstates describes the Uemura relation for 2D superconductors.
机译:最近,Gomes等人。 [1]已经可视化了高T_c超导体Bi_2Sr_2CaCu_2O_ {8+ \ delta}中临界温度T_c以上的纳米级区域(NRs)中的间隙形成。已经发现,随着温度降低,NRs在由不均匀性组成的本体超导状态下膨胀。不均匀性[2]的大小接近于NR [1]的最小大小这一事实导致以下结论:超导阶段是这些NR重叠的结果。在本文中,我们对NR进行了电荷和渗流状态分析,结果表明,在第一个临界掺杂x_ {c1}时,当超导开始时,每个NR都携带一个以电子电荷为单位的正电荷,因此我们将NR归因于单孔玻色子,连接这些玻色子的渗流线出现。在第二次临界掺杂x_ {c2}处,当超导消失时,我们的分析表明每个NR的电荷等于2。 x_ {c2}的起源可以通过在NRs中引入其他正相孔费米子来理解,它们的浓度随x_ {c1}的出现而随着掺杂的增加而平稳增加,并破坏玻色子在x_ {c2}处的渗透线。最后一个导致伪间隙(PG)区的整体玻色子特性消失,这解释了能斯特效应中涡旋存在的上限[3]。[1]由于证明了PG边界处不存在NR,因此可以得出结论:沿着该边界以及在x_ {c2}中,所有的玻色子都消失了。作为单个玻色子出现的理由,2Dfermions的玻色化已通过任意子的概念得到严格证明。激发的铁离子基态和玻色子基态之间能隙的线性密度依赖性描述了二维超导体的Uemura关系。

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