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Oxygen-isotope effect on density wave transitions in La$_3$Ni$_2$O$_{7}$

Rustem Khasanov, Vahid Sazgari, Igor Plokhikh, Lifen Shi, KeYuan Ma, Marisa Medarde, Ekaterina Pomjakushina, Tomasz Klimczuk, Thomas J. Hicken, Hubertus Luetkens, Christof W. Schneieder, Zurab Guguchia, Sergey Medvedev, Dariusz J. Gawryluk

Abstract

TThe isotope effect is a powerful probe of electron-phonon interactions in solid-state systems, offering key insights into how atomic mass influences emergent quantum states. Here, the impact of oxygen isotope substitution ($^{16}{\rm O}\rightarrow \; ^{18}{\rm O}$) on charge- and spin-density wave (CDW and SDW) transitions in the double-layer Ruddlesden-Popper nickelate La$_3$Ni$_2$O$_7$ is investigated. A clear isotope effect is observed in the CDW transition: the transition temperature ($T_{\rm CDW}$) increases upon $^{18}$O substitution. In contrast, the SDW transition temperature remains unaffected within experimental uncertainty. These findings point to a strong involvement of lattice vibrations in the formation of charge order, while spin order appears to be predominantly of electronic origin. The results suggest that electron-phonon coupling, manifested through the CDW response to isotope substitution, may be relevant to the superconducting pairing mechanism in Ruddlesden-Popper nickelates.

Oxygen-isotope effect on density wave transitions in La$_3$Ni$_2$O$_{7}$

Abstract

TThe isotope effect is a powerful probe of electron-phonon interactions in solid-state systems, offering key insights into how atomic mass influences emergent quantum states. Here, the impact of oxygen isotope substitution () on charge- and spin-density wave (CDW and SDW) transitions in the double-layer Ruddlesden-Popper nickelate LaNiO is investigated. A clear isotope effect is observed in the CDW transition: the transition temperature () increases upon O substitution. In contrast, the SDW transition temperature remains unaffected within experimental uncertainty. These findings point to a strong involvement of lattice vibrations in the formation of charge order, while spin order appears to be predominantly of electronic origin. The results suggest that electron-phonon coupling, manifested through the CDW response to isotope substitution, may be relevant to the superconducting pairing mechanism in Ruddlesden-Popper nickelates.

Paper Structure

This paper contains 1 equation, 3 figures, 1 table.

Figures (3)

  • Figure 1: (a) Room-temperature Raman spectra of oxygen-isotope substituted La$_3$Ni$_2$O$_7$ samples. Solid lines represent fits using seven Lorentzian functions. Dashed lines indicate the peak positions. (b) The oxygen participation parameter $f_{\rm O}$ as a function of the Raman wavenumber $^{16}\nu$.
  • Figure 2: (a) Raw resistivity curves of the $^{16}$O/$^{18}$O-substituted La$_3$Ni$_2$O$_7$ samples. (b) Extended view of the first derivatives of the resistivity data in the vicinity of the CDW transitions. The red and blue numbers correspond to the CDW transition temperatures of La$_3$Ni$_2\,^{16}$O$_7$ and La$_3$Ni$_2\,^{18}$O$_7$, determined using different criteria (see text for details).
  • Figure 3: (a) Temperature dependence of the magnetic volume fraction $f_{\rm m}$ for $^{16}$O- and $^{18}$O-substituted La$_3$Ni$_2$O$_7$ and La$_4$Ni$_3$O$_{10}$ samples. (b) Extended view of the $f_{\rm m}(T)$ curves in the vicinity of the SDW transitions. The vertical dashed lines and grey stripe indicate the CDW and SDW transition temperatures ($T_{\rm CDW}$ and $T_{\rm SDW}$), as reported in the literature.Chen_PRL_2024Khasanov_NatPhys_La327_2025Chen_arxiv_2024Zhang_NatCom_2020Khasanov_arxiv_La4310_2025Liu_NatCom_2024Wang_ChinPhysLett_2024Wang_InorgChem_2024Wu_PRB_2001Liu_SciChina_2023Seo_InorgChem_1996