Glittum Cecilie, Štrkalj Antonio, Prabhakaran Dharmalingam, Goddard Paul A, Batista Cristian D, Castelnovo Claudio
T.C.M. Group, Cavendish Laboratory, University of Cambridge, Cambridge, UK.
Department of Physics, Faculty of Science, University of Zagreb, Zagreb, Croatia.
Nat Phys. 2025;21(8):1211-1216. doi: 10.1038/s41567-025-02923-8. Epub 2025 May 29.
Ideas about resonant valence bond liquids and spin-charge separation have led to key concepts in physics such as quantum spin liquids, emergent gauge symmetries, topological order and fractionalization. Despite extensive efforts to demonstrate the existence of a resonant valence bond phase in the Hubbard model that originally motivated the concept, a definitive realization has yet to be achieved. Here we present a solution to this long-standing problem by uncovering a resonant valence bond phase exhibiting spin-charge separation in realistic Hamiltonians. We show analytically that this ground state emerges in the dilute-doping limit of a half-filled Mott insulator on corner-sharing tetrahedral lattices with frustrated hopping, in the absence of exchange interactions. We confirm numerically that the results extend to finite exchange interactions, finite-sized systems and finite dopant density. Although much attention has been devoted to the emergence of unconventional states from geometrically frustrated interactions, our work demonstrates that kinetic energy frustration in doped Mott insulators may be essential for stabilizing robust, topologically ordered states in real materials.
关于共振价键液体和自旋-电荷分离的观点引出了物理学中的关键概念,如量子自旋液体、涌现规范对称性、拓扑序和分数化。尽管人们付出了巨大努力,试图在最初激发这一概念的哈伯德模型中证明共振价键相的存在,但尚未实现明确的成果。在此,我们通过揭示一种在现实哈密顿量中表现出自旋-电荷分离的共振价键相,给出了这个长期存在问题的解决方案。我们通过分析表明,在没有交换相互作用的情况下,这种基态出现在具有受挫跳跃的角共享四面体晶格上半填充莫特绝缘体的稀掺杂极限中。我们通过数值计算证实,结果适用于有限的交换相互作用、有限尺寸的系统和有限的掺杂剂密度。尽管人们对几何受挫相互作用产生的非常规态给予了很多关注,但我们的工作表明,掺杂莫特绝缘体中的动能受挫对于在实际材料中稳定稳健的拓扑有序态可能至关重要。