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Observation of Orbital-Selective Dual Modulations in an Anisotropic Antiferromagnetic Kagome Metal TbTi3Bi4

Renjie Zhang1,2,3, Bocheng Yu4, Hengxin Tan5, Yiwei Cheng6,1, Feiran Shen7, Junye Yang7, Dan Mu8, Xinru Han1,9, Alfred Zong10 et al.

Quanxin Hu1, Xuezhi Chen6,1, Yudong Hu1, Chengnuo Meng6, Junchao Ren6, Junqin Li6, Zhenhua Chen6, Zhengtai Liu6, Mao Ye6, Makoto Hashimoto11, Donghui Lu11, Shifeng Jin2,3, Binghai Yan12, Lunhua He2,7,13, Ziqiang Wang14, Tian Shang4,*, Yaobo Huang6,†, Baiqing Lv1,5,15,‡, and Hong Ding1,16,17

  • *Contact author: tshang@phy.ecnu.edu.cn
  • †Contact author: huangyaobo@sari.ac.cn
  • ‡Contact author: baiqing@sjtu.edu.cn

Phys. Rev. X 15, 031012 – Published 10 July, 2025

DOI: https://doi.org/10.1103/c3tg-1lxl

Abstract

Orbital selectivity is pivotal in dictating the phase diagrams of multiorbital systems, with prominent examples including the orbital-selective Mott phase and superconductivity. The intercalation of anisotropic layers represents an effective method for enhancing orbital selectivity and thereby shaping the low-energy physics of multiorbital systems. Despite its potential, related experimental studies, especially those elucidating the correlation between orbital selectivity and magnetism, remain limited. In this work, we systematically examine the interplay between orbital selectivity and magnetism in the newly discovered anisotropic kagome TbTi3Bi4 single crystal, and report the coexistence of orbital-selective dual-band modulations (q1∼1/3a*, q2∼0.28b*) within the antiferromagnetic (AFM) state. By combining soft x-ray and vacuum ultraviolet angle-resolved photoemission spectroscopy measurements, neutron powder diffraction, scanning tunneling microscopy, and density-functional-theory calculations, we identify these dual-band reconstructions as manifestations of the AFM order driven by a (approximately 1/3, 0.28, 0) nesting instability of the intercalated Tb 5dxz orbitals. These orbital-selective modulations induce unusual momentum-dependent band folding and lead to the emergence of Dirac cones only at the M¯1 point, signaling a topological phase transition in the AFM state. Importantly, the discovery of orbital-selective (approximately 1/3, 0.28, 0) AFM order offers crucial insights into the mechanism underlying the fractional magnetization plateau in this kagome AFM metal. Our findings not only underscore the essential role of both conducting and localized electrons in determining the magnetic orders of LnTi3Bi4 (Ln=lanthanide) kagome metals but also offer a pathway for manipulating magnetism through selective control of anisotropic electronic structures.

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