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Density waves in low-pressure bilayer nickelates

Published 28 Jun 2026 in cond-mat.str-el and cond-mat.supr-con | (2606.29527v1)

Abstract: The low-pressure phase diagram of La<em>3<em>3Ni2_2O7_7 provides an important reference for understanding its pressure-induced high-temperature superconductivity. While the spin-density-wave transition at T</em>SDW150T</em>{\text{SDW}}\approx150 K is increasingly well established, the origin of the second density-wave transition at TDW130T_{\text{DW}}\approx130 K has remained unresolved. Here, we perform unrestricted Hartree-Fock calculations to investigate the potential origin of the second transition. {Within the orthorhombic phase, the degeneracy between possible ordering wavevectors at Q<em>Y=(0,π)\boldsymbol{Q}<em>{Y}=(0,π) and at Q</em>X=(π,0)\boldsymbol{Q}</em>{X}=(π,0) is lifted and the electronic system} develops a double-stripe spin-density wave with ordering vector QY=(0,π)\boldsymbol{Q}_{Y}=(0,π). We identify that the pure double stripe spin state is unstable in La3_3Ni2_2O7_7 towards a commensurate charge-density wave instability, which favors a spin-modulated double stripe order with intertwined charge and spin instabilities and establish the hierarchy of ordered states in La3_3Ni2_2O7_7, providing an important link between its ambient-pressure and superconducting high-pressure phases. We further discuss our results in the context of available experimental literature and propose further experimental tests to elucidate the origin of the SDW/DW states in this system.

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