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在磁场中 YbPtPb 中的自旋子限制和尖锐的纵向模式。

Spinon confinement and a sharp longitudinal mode in YbPtPb in magnetic fields.

机构信息

Department of Physics and Astronomy, Texas A&M University, College Station, TX, 77843, USA.

Stewart Blusson Quantum Matter Institute, University of British Columbia, Vancouver, BC, V6T 1Z4, Canada.

出版信息

Nat Commun. 2019 Mar 8;10(1):1123. doi: 10.1038/s41467-019-08715-y.

DOI:10.1038/s41467-019-08715-y
PMID:30850591
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6408591/
Abstract

The fundamental excitations in an antiferromagnetic chain of spins-1/2 are spinons, de-confined fractional quasiparticles that when combined in pairs, form a triplet excitation continuum. In an Ising-like spin chain the continuum is gapped and the ground state is Néel ordered. Here, we report high resolution neutron scattering experiments, which reveal how a magnetic field closes this gap and drives the spin chains in YbPtPb to a critical, disordered Luttinger-liquid state. In YbPtPb the effective spins-1/2 describe the dynamics of large, Ising-like Yb magnetic moments, ensuring that the measured excitations are exclusively longitudinal, which we find to be well described by time-dependent density matrix renormalization group calculations. The inter-chain coupling leads to the confinement of spinons, a condensed matter analog of quark confinement in quantum chromodynamics. Insensitive to transverse fluctuations, our measurements show how a gapless, dispersive longitudinal mode arises from confinement and evolves with magnetic order.

摘要

在一个自旋为 1/2 的反铁磁链中的基本激发是自旋子,它们是解缠的分数准粒子,当它们成对结合时,形成一个三重激发连续体。在类伊辛自旋链中,连续体是带隙的,基态是奈尔有序的。在这里,我们报告了高分辨率的中子散射实验,这些实验揭示了磁场如何关闭这个带隙,并驱动 YbPtPb 中的自旋链进入一个临界的无序的 Luttinger 液体状态。在 YbPtPb 中,有效自旋为 1/2,描述了大的,类伊辛的 Yb 磁矩的动力学,这确保了测量到的激发是纯粹的纵向的,我们发现这可以很好地用时间相关的密度矩阵重整化群计算来描述。链间耦合导致了自旋子的束缚,这是量子色动力学中夸克束缚的凝聚态类比。我们的测量对横向涨落不敏感,它们展示了无带隙的、色散的纵向模式如何从束缚中产生,并随着磁序的演化而演化。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/c9c0b14403eb/41467_2019_8715_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/5fc67def7772/41467_2019_8715_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/9b44b161afa7/41467_2019_8715_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/c7813b0592bf/41467_2019_8715_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/c9c0b14403eb/41467_2019_8715_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/5fc67def7772/41467_2019_8715_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/9b44b161afa7/41467_2019_8715_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/c7813b0592bf/41467_2019_8715_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/efdc/6408591/c9c0b14403eb/41467_2019_8715_Fig4_HTML.jpg

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