Source capture
Authors Shu Cai, Yuqing Tian, Shengjun Yan, Jinyu Zhao, Bo Hao, Jianfeng Zhang, Shuaihang Sun, Yang Ding, Qi Wu, Ho-kwang Mao, I. Bozovic, Yuefeng Nie, Liling Sun
Relevance score 5.420
Primary category cond-mat.supr-con
Published 2026-08-04
Research paradigm Not available in this batch.
Sample form Not available in this batch.

Summary

Researchers have prepared freestanding La0.8Sr0.2NiO2 thin films and performed electrical resistance measurements using a diamond anvil cell at ultrahigh pressures up to 210 GPa. The experiments reveal a dome-shaped evolution of the superconducting onset transition temperature: beginning at approximately 16 K at ambient pressure, it rises monotonically with increasing pressure, reaches a peak of 74.5 K at 146 GPa, and then slowly decreases while still retaining 57.4 K at 210 GPa. Through derivative analysis and magnetic field suppression experiments, it is confirmed that this enhancement in transition temperature stems from an intrinsic strengthening of superconductivity, rather than a simple broadening of the transition width. A comparison with Nd0.85Sr0.15NiO2 films shows that both exhibit a linear increase with pressure below 60 GPa with similar slopes, though their behaviors diverge at higher pressures; nonetheless, the maximum onset temperature for both is approximately 75 K, indicating that the NiO2 planes dominate the superconductivity and that the magnetic moments of rare-earth f orbitals have minimal influence. This work represents the first observation of robust superconductivity in oxide superconductors over such a wide pressure range, demonstrating that the pairing strength in infinite-layer nickelates remains unsuppressed under extreme compression, and provides important clues for understanding the mechanism of unconventional superconductivity.

Materials

Not available in this batch.

Methods

Not available in this batch.

Keywords

Not available in this batch.

Highlights

Not available in this batch.

Conclusions

Not available in this batch.

Main claims

  • Superconductivity in freestanding La0.8Sr0.2NiO2 membranes is robust up to 210 GPa with a dome-like Tc onset, peaking at 74.5 K at 146 GPa.
    • Evidence: Fig. 2c–f: R(T) at various pressures show persistent resistive drops; Tc[onset] values extracted and plotted in Fig. 5.
  • The enhancement is intrinsic, not due to transition broadening, as evidenced by derivative analysis and magnetic field suppression.
    • Evidence: Fig. 3: dR/dT analysis shows Tc[m] increases significantly; Fig. 4: Hc2 enhanced at 80 GPa.
  • Comparison with Nd0.85Sr0.15NiO2 shows both peak near 75 K, indicating NiO2 planes govern superconductivity with little influence from rare-earth f-orbitals.
    • Evidence: Fig. 5 includes Nd data; both maxima ≈75 K at different pressures; text states f-orbital moment has little impact.
  • This robustness is unprecedented among high-Tc oxide superconductors, with most systems suppressed at much lower pressures.
    • Evidence: Fig. 5 comparative data: cuprates, bismuthates suppressed below 40 GPa; text mentions only infinite-layer nickelates persist above 200 GPa.

Workflow

  • freestanding_membrane_preparation — Freestanding single-crystal La0.8Sr0.2NiO2 membranes are successfully synthesized.
    • Materials: La0.8Sr0.2NiO3 perovskite thin film; SrTiO3 substrate; Sr4Al2O7 sacrificial layer; CaH2 reductant
    • Methods: molecular-beam epitaxy; topotactic reduction; chemical release in deionized water
    • Observations: highly oriented (00l) XRD peaks; superconducting transition at ≈16 K before transfer
  • high_pressure_device_assembly — Membranes are integrated into DAC devices for high-pressure resistance measurements.
    • Materials: freestanding membrane; diamond anvil cell; gold electrodes
    • Methods: micromanipulator transfer onto diamond culet; electrode deposition
    • Observations: optical image of membrane with four electrodes
  • high_pressure_resistance_measurements — Superconducting transition persists up to 210 GPa, with Tc[onset] exhibiting a dome-like pressure dependence.
    • Materials: La0.8Sr0.2NiO2 membrane devices
    • Methods: resistivity measurement under pressure; magnetic field application up to 7T
    • Observations: resistance drops at Tc[onset] values; Tc[onset] increases with pressure up to 146 GPa then decreases
  • data_analysis — The increase in Tc[onset] reflects genuine strengthening of superconductivity, not just broadening.
    • Materials: R(T) data; dR/dT curves; magnetic field sweeps
    • Methods: two-line intersection method for Tc[onset]; derivative analysis for Tc[m]; upper critical field determination
    • Observations: Tc[m] increases fourfold; transition width increases but cannot account for Tc[onset] shift; Hc2 enhanced under pressure
  • interpretation — Infinite-layer nickelates exhibit uniquely robust superconductivity under extreme compression, dominated by NiO2 planes.
    • Materials: phase diagram data from multiple samples and literature
    • Methods: construction of P-T phase diagram; comparison with Nd0.85Sr0.15NiO2 and other superconductors
    • Observations: dome-like behavior with maximum 74.5 K at 146 GPa; both La and Nd nickelates peak at ≈75K; other oxides show suppression at much lower pressures