摘要
研究人员利用高质量La3Ni2O7单晶,通过精确测量面内和面外电阻率,建立了高精度的压力–温度相图。他们分辨出两个具有不同压力依赖性的密度波相关异常:其中低温异常T1先被压制,在约10 GPa结构相变后急剧增强,而高温自旋密度波异常T2则单调升高。压力诱导的结构转变不仅增大了两方向电阻率,还显著增强了低温电阻率各向异性,表明密度波序对电荷动力学有深刻影响。一旦压力将密度波相完全压制,在相边界处出现零电阻超导,其起始温度达68 K,正常态电阻率在超导转变温度以上至300 K的宽温区内呈线性温度关系,散射率落入普朗克极限范围。这些结果说明压力通过调控密度波序,重构了各向异性电荷输运,进而产生强散射的奇异金属态和超导电性,确立了密度波关联和普朗克耗散是La3Ni2O7的显著特征。
材料
方法
- high-pressure resistivity measurements
- Montgomery method for anisotropic transport
- synchrotron X-ray diffraction
- transmission electron microscopy
- scanning electron microscopy
- energy-dispersive X-ray spectroscopy
- Laue diffraction
- single crystal X-ray diffraction
- structural refinement
关键词
- density wave order
- spin density wave
- charge order
- planckian dissipation
- strange metal
- temperature linear resistivity
- resistivity anisotropy
- pressure induced structural transition
- superconductivity
- quantum critical fluctuations
亮点
- High-quality, oxygen-stoichiometric, stacking-fault-free La3Ni2O7 single crystals are synthesized for the first time.
- The low-temperature density-wave anomalyT1 does not vanish below 10 GPa but is abruptly enhanced across the structural transition.
- The transport anisotropy increases dramatically at low temperatures upon entering the tetragonal phase, driven by the density‑wave order.
- The normal‑state T‑linear resistivity slope and Fermi velocity place La3Ni2O7 in the Planckian dissipation regime, similar to other strange metals.
- The pressure–temperature phase diagram is highly reproducible across several single crystals, confirming the intrinsic nature of the electronic modifications.
结论
- Two distinct density-wave anomalies, T1 and T2, are resolved: T1 is initially suppressed and then sharply enhanced after the structural transition, while T2 (spin-density-wave) increases monotonically with pressure.
- The orthorhombic-to-tetragonal structural transition enhances both in-plane and out-of-plane resistivities and strongly increases low-temperature resistivity anisotropy due to the density-wave order.
- Superconductivity with zero resistance emerges near the boundary where the density-wave phases are fully suppressed, with an onset Tc up to 68 K.
- Above Tc, the normal-state resistivity displays a T‑linear dependence over a wide temperature range, and the extracted scattering rate lies within the Planckian limit, revealing a strange‑metal state.
- Robust density-wave correlations and Planckian dissipation are defining features of La3Ni2O7, and superconductivity develops from this strongly correlated normal state.
主要论断
- Two distinct density-wave-related anomalies (T1 and T2) exhibit contrasting pressure dependences, with T1 enhanced after a structural transition.
- 证据: Temperature derivative of in-plane resistivity shows T1 and T2 anomalies,Phase diagram Fig. 2e shows T1 initially suppressed then sharply increased near 10 GPa, T2 monotonically increasing
- The pressure-induced structural transition enhances low-temperature resistivity and its anisotropy.
- 证据: At ≈8-10 GPa, ρab and ρc increase at low T, and ρc/ρab rises sharply below 150 K (Figs. 3,4a),The change coincides with orthorhombic-to-tetragonal transition
- Zero-resistance superconductivity emerges near the boundary where density-wave phases are fully suppressed.
- 证据: Tc onset and Tc zero appear at pressures >14 GPa where T1, T2 and resistivity upturn disappear (Fig. 2e),Tc onset up to 68 K, zero resistance up to 55 K at 20 GPa
- The normal-state resistivity above Tc exhibits T-linear dependence and Planckian dissipation.
- 证据: ρab is T-linear from ≈80 K to 300 K at 18 and 20 GPa with small residual resistivity (Fig. 4f),Scattering rate α ≈ 1.6 ± 0.4, close to Planckian limit (Fig. 4c)
研究流程
- sample_preparation — High-quality oxygen-stoichiometric bilayer La3Ni2O7 single crystals were obtained.
- 材料: La2O3 (99.99%); NiO (99.99%); flux; oxygen agent
- 方法: high-pressure growth in cubic-anvil press at 3 GPa; heating at 1373 K then slow cooling to 1073K; X-ray diffraction; Laue diffraction; STEM and EDS mapping
- 观察: large single crystals up to 220 μm; orthorhombic Am2m structure; no oxygen vacancies; no stacking faults; homogeneous element distribution
- measurement — Pressure-dependent resistivity and anisotropy reveal density-wave anomalies and superconductivity.
- 材料: single crystal samples 2#-a, 2#-d, 2#-e; silver epoxy or nanoparticle silver paste electrodes; Daphne 7575/7676 pressure transmitting medium; cubic-anvil press; PPMS
- 方法: four-contact resistivity measurements; Montgomery method for anisotropy; in-plane (ab) and out-of-plane (c) resistivity under pressure
- 观察: ρab decreases with P at 300 K, then develops semiconducting upturn at intermediate P; two anomalies T1 and T2 in resistivity derivative; resistivity anisotropy ρc/ρab increases sharply at low T near 10 GPa; superconducting transition with Tc onset up to 68 K and zero resistance up to 55 K at 20 GPa
- analysis — Density-wave orders are modified by pressure, and the normal state at high pressure exhibits Planckian dissipation.
- 方法: temperature derivative of resistivity to identify characteristic temperatures; Drude model to extract scattering rate; comparison with Planckian limit α = (ħ/τ)/(k_B T); construction of P-T phase diagram
- 观察: T1 initially suppressed then sharply increased around 10 GPa (structural transition); T2 increases monotonically with pressure; T-linear ρab from ≈80 K to 300 K at 18-20 GPa with slope ≈0.28 μΩ cm/K; scattering rate α ≈ 1.6 ± 0.4, close to Planckian limit
- interpretation — Superconductivity in La3Ni2O7 develops from a strongly correlated state with Planckian dissipation when robust density-wave orders are fully suppressed.
- 观察: superconductivity emerges only after full suppression of T1, T2, and resistivity upturn; strange-metal state with T-linear resistivity and strong scattering