论文标题

通过语音子的拉曼散射在量子自旋冰中探测出来的QED:浅弹性散射和配对的产生

Probing emergent QED in quantum spin ice via Raman scattering of phonons: shallow inelastic scattering and pair production

论文作者

Seth, Arnab, Bhattacharjee, Subhro, Moessner, Roderich

论文摘要

我们提出了一种用于声子拉曼散射的新机制,该机制基于非kramers磁离子中存在的线性磁弹性耦合。这提供了拉曼活性声子与磁铁的准粒子的直接耦合。我们建议使用这种机制探测U(1)量子旋转液体的新兴磁性单极,电荷和光子的光子和光子,称为量子自旋冰。在候选稀土pyrochlore材料中检测到这一点是一项艰巨的任务。我们表明,声子的拉曼散射横截面直接产生相关信息,随着声子宽度的扩展,我们对其进行了计算,表现出特征性的频率依赖性,反映了出现激励状态的两粒子密度。值得注意的是,我们发现拉曼线宽对对称分数化的细节很敏感,因此可以揭示有关量子旋转液体中对称性实现的信息的信息,从而为$π$ -Flux阶段提供了诊断。因此,声子的拉曼散射提供了一种有用的实验工具,可以探测量子自旋液体中的分数化,该工具与量子电动力学和量子染色体动力学的深度无弹性散射紧密相关。的确,后者的差异比技术性更大:由于渐近自由而在高能中出现了partons(夸克),而临时性的偏差是由低能量下的旋转的分数产生的。

We present a new mechanism for Raman scattering of phonons, which is based on the linear magnetoelastic coupling present in non-Kramers magnetic ions. This provides a direct coupling of Raman-active phonons to the magnet's quasiparticles. We propose to use this mechanism to probe the emergent magnetic monopoles, electric charges, and photons of the emergent quantum electrodynamics (eQED) of the U(1) quantum spin liquid known as quantum spin ice. Detecting this eQED in candidate rare-earth pyrochlore materials, or indeed signatures of topological magnetic phases more generally, is a challenging task. We show that the Raman scattering cross-section of the phonons directly yields relevant information, with the broadening of the phonon linewidth, which we compute, exhibiting a characteristic frequency dependence reflecting the two-particle density of states of the emergent excitations. Remarkably, we find that the Raman linewidth is sensitive to the details of the symmetry fractionalisation and hence can reveal information about the projective implementation of symmetry in the quantum spin liquid, thereby providing a diagnostic for a $π$-flux phase. The Raman scattering of the phonons thus provides a useful experimental tool to probe the fractionalisation in quantum spin liquids that turns out closely to mirror pair production in quantum electrodynamics and the deep inelastic scattering of quantum chromodynamics. Indeed, the difference to the latter is conceptual more than technical: the partons (quarks) emerge from the hadrons at high energies due to asymptotic freedom, while those in eQED arise from fractionalisation of the spins at low energies.

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