Source capture, zotero
Authors Qi-Yi Wu, De-Yuan Hu, Chen Zhang, Hao Liu, Bo Chen, Ying Zhou, Zhong-Tuo Fu, Chun-Hui Lv, Zi-Jie Xu, Hai-Long Deng, Meng-Wu Huo, H. Y. Liu, Jun Liu, Yu-Xia Duan, Dao-Xin Yao, Meng Wang, Jian-Qiao Meng
Relevance score 5.710
Primary category cond-mat.str-el
Published 2026-01-05
Research paradigm Experimental
Sample form Single Crystal

Summary

Using polarized ultrafast pump-probe spectroscopy, the researchers comparatively investigated the normal-state electronic dynamics of bilayer La3Ni2O7 and trilayer La4Ni3O10 single crystals under ambient pressure. Both materials exhibit a density-wave transition accompanied by the opening of a quasiparticle relaxation bottleneck, yet their electronic responses display markedly different symmetries: trilayer La4Ni3O10 remains optically isotropic across the entire temperature range, whereas bilayer La3Ni2O7 shows clear twofold (C2) rotational symmetry breaking—i.e., electronic nematicity—at low temperatures. This nematicity manifests in the anisotropy of slow quasiparticle relaxation dynamics and effective gap scale, and below 115 K it competes with a secondary isotropic order, leading to a non-monotonic temperature dependence of the nematic signal. This work reveals the presence of electronic nematic fluctuations in bilayer nickelates, which are absent in the trilayer system, suggesting a close relationship between electronic nematicity and high-pressure superconducting pairing in La3Ni2O7, thereby providing key insights into the microscopic mechanism of this class of nickel-based superconductors.

Materials

Methods

  • Polarized ultrafast pump-probe spectroscopy
  • Rothwarf-Taylor model fitting
  • polarized ultrafast pump-probe spectroscopy

Keywords

  • electronic nematicity
  • density wave transition
  • quasiparticle relaxation bottleneck
  • twofold rotational symmetry breaking
  • c2 symmetry
  • c2 anisotropy

Highlights

  • The presence of macroscopic electronic anisotropy in the bilayer system, and its absence in the trilayer system, suggests an intimate relation between electronic nematic fluctuations and superconducting pairing in La3Ni2O7.
  • This nematicity manifests as a significant anisotropy in the slow quasiparticle relaxation dynamics and effective gap scales.
  • Electronic nematicity revealed by polarized ultrafast spectroscopy in bilayer La3Ni2O7.
  • The twofold anisotropy and competition with isotropic order provide deeper exploration for superconducting pairing.

Conclusions

  • La3Ni2O7 exhibits a pronounced rotational-symmetry-breaking electronic response with twofold anisotropy, indicating electronic nematicity.
  • The non-monotonic temperature dependence of the nematic signal indicates its competition with a secondary, isotropic density-wave-like order below 115 K.
  • La4Ni3O10 maintains a robustly isotropic optical response over the entire temperature range, showing no nematicity.
  • La4Ni3O10 maintains an isotropic optical response across the entire temperature range.
  • La3Ni2O7 exhibits a pronounced twofold (C2) anisotropy in its low-temperature electronic dynamics.
  • This electronic nematicity competes with a secondary isotropic order emerging below 115 K.
  • The presence of macroscopic electronic anisotropy in the bilayer system and its absence in the trilayer system suggests an intimate relation between electronic nematic fluctuations and superconducting pairing in La3Ni2O7.

Main claims

  • Bilayer La3Ni2O7 exhibits electronic nematicity with twofold (C2) rotational symmetry breaking at low temperatures, while trilayer La4Ni3O10 remains isotropic.
    • Evidence: Abstract: 'La3Ni2O7 shows clear twofold (C2) rotational symmetry breaking—i.e., electronic nematicity—at low temperatures'
  • The nematicity competes with a secondary isotropic order emerging below 115 K, leading to a non-monotonic temperature dependence of the nematic signal.
    • Evidence: Abstract: 'below 115 K it competes with a secondary isotropic order, leading to a non-monotonic temperature dependence of the nematic signal'
  • La3Ni2O7 exhibits a pronounced twofold (C2) anisotropy in its low-temperature electronic dynamics, indicative of electronic nematicity.
    • Evidence: Normalized transient reflectivity (ΔR/R)_Norm shows clear deviation between φ=0° and φ=90° below T_SDW.,Polar plots of τ_s show isotropic at 160 K, two-fold at 115 K and 70 K.,Difference plot τ_ani = τ_s0 - τ_s90 peaks near 115 K.
  • The electronic nematicity in La3Ni2O7 competes with a secondary isotropic order emerging below 115 K.
    • Evidence: τ_ani shows non-monotonic behavior: increases below T_SDW, peaks near 115 K, then decreases upon further cooling.,Optical measurements report opening of an energy gap below 115 K, possibly associated with CDW order.
  • La4Ni3O10 maintains an isotropic optical response across the entire temperature range, showing no rotational symmetry breaking.
    • Evidence: (ΔR/R)_Norm curves for φ=0° and φ=90° completely overlap at all temperatures.,Polar plots of τ_s remain circular at all measured temperatures (130 K, 115 K, 70 K).
  • The presence of electronic nematicity in bilayer La3Ni2O7 and its absence in trilayer La4Ni3O10 suggests an intimate relation between nematic fluctuations and superconducting pairing in La3Ni2O7.
    • Evidence: Nematicity in iron-based and cuprate superconductors is linked to enhanced Tc near a nematic quantum critical point.,The observed anisotropy is spin-driven (SDW gap) and may provide additional attractive interaction for pairing.

Workflow

  • Sample preparation
    • Materials: La3Ni2O7 and La4Ni3O10 single crystals
    • Methods: Vertical optical image floating-zone method; Cleavage of (001) planes
    • Observations: High-quality single crystals with well-defined surfaces
  • Ultrafast pump-probe spectroscopy
    • Materials: Single crystals
    • Methods: Polarized ultrafast pump-probe measurement; Rotation of half-wave plate and polarizer
    • Observations: Normalized transient reflectivity along 0° and 90°
  • Data analysis — Bilayer exhibits electronic nematicity that competes with isotropic order below 115K
    • Materials: Transient reflectivity data
    • Methods: Two-exponential decay model; Rothwarf-Taylor model
    • Observations: La3Ni2O7 shows C2 rotational symmetry breaking below SDW transition; La4Ni3O10 remains isotropic
  • sample_preparation
    • Materials: La3Ni2O7 single crystals; La4Ni3O10 single crystals
    • Methods: vertical optical image floating-zone method
  • measurement
    • Materials: single crystals of La3Ni2O7 and La4Ni3O10
    • Methods: polarized ultrafast pump-probe spectroscopy
    • Observations: normalized transient reflectivity (ΔR/R)_Norm measured as function of delay time; angular dependence of (ΔR/R)_Norm and relaxation times
  • analysis
    • Materials: measured ΔR/R data
    • Methods: two-exponential decay model fitting; Rothwarf-Taylor (RT) model fitting for gap extraction
    • Observations: τ_f and τ_s extracted for both polarizations; temperature dependence of τ_f and τ_s; difference plots (ΔR/R)_ani and τ_ani = τ_s0 - τ_s90
  • interpretation — La3Ni2O7 exhibits electronic nematicity (C2 rotational symmetry breaking) in its low-temperature electronic dynamics, while La4Ni3O10 remains isotropic.
    • Methods: comparison of symmetry properties between La3Ni2O7 and La4Ni3O10; analysis of rotational symmetry using polar plots of τ_s
    • Observations: La4Ni3O10: isotropic response across all temperatures; La3Ni2O7: isotropic at high T, pronounced two-fold (C2) anisotropy below T_SDW ≈140K; non-monotonic τ_ani peaking near 115 K, suppressed by secondary isotropic order below 115K