Liu Ruixian, Stone Matthew B, Gao Shang, Nakamura Mitsutaka, Kamazawa Kazuya, Krajewska Aleksandra, Walker Helen C, Cheng Peng, Yu Rong, Si Qimiao, Dai Pengcheng, Lu Xingye
Center for Advanced Quantum Studies, School of Physics and Astronomy, Beijing Normal University, Beijing, China.
Key Laboratory of Multiscale Spin Physics, Ministry of Education, Beijing, China.
Nat Commun. 2025 Jun 5;16(1):5212. doi: 10.1038/s41467-025-60071-2.
The quantum-disordered state in FeSe, intertwined with superconductivity and nematicity, has been a research focus in iron-based superconductors. However, the intrinsic spin excitations across the entire Brillouin zone in detwinned FeSe, crucial for understanding its magnetism and superconductivity, have remained unresolved. Using inelastic neutron scattering, we reveal that stripe spin excitations (Q = (1, 0)/(0, 1)) exhibit the C symmetry, while Néel spin excitations (Q = (1, 1)) retain C symmetry within the nematic state. Temperature-dependent differences between Q = (1, 0) and (0, 1) spin excitations above the structural transition unambiguously reveals the nematic quantum disordered state. Comparison with NaFeAs suggests the Néel excitations originate from enhanced 3d orbital correlations. Modeling the stripe dispersions using a J-K-J Heisenberg Hamiltonian, we establish a spin-interaction phase diagram, positioning FeSe near a crossover regime between the antiferroquadrupolar, Néel, and stripe orders. Our results provide key insights into the microscopic spin interactions and their role in the intertwined orders in iron-based superconductors.
铁硒(FeSe)中的量子无序态与超导性和向列性相互交织,一直是铁基超导体的研究重点。然而,对于理解其磁性和超导性至关重要的去孪晶铁硒中整个布里渊区的本征自旋激发仍未得到解决。利用非弹性中子散射,我们发现条纹自旋激发(Q = (1, 0)/(0, 1))呈现C对称性,而奈尔自旋激发(Q = (1, 1))在向列态内保持C对称性。结构转变温度以上,Q = (1, 0)和(0, 1)自旋激发之间的温度依赖性差异明确揭示了向列量子无序态。与砷化钠铁(NaFeAs)的比较表明,奈尔激发源于增强的3d轨道相关性。使用J - K - J海森堡哈密顿量对条纹色散进行建模,我们建立了一个自旋相互作用相图,将铁硒置于反铁四极、奈尔和条纹序之间的交叉区域附近。我们的结果为微观自旋相互作用及其在铁基超导体中相互交织序中的作用提供了关键见解。