- The paper identifies a d-wave gap in electron-doped Sr₂IrO₄, mirroring the dual-phase behavior seen in cuprate superconductors.
- Employing ARPES and innovative in situ potassium deposition, the study precisely maps the Fermi surface and temperature-dependent gap variations.
- The findings highlight heterogeneous gap profiles at nodes and antinodes, offering insights into the interplay between pseudogap phenomena and potential superconducting correlations.
Observation of a d-wave Gap in Electron-Doped Sr2IrO4
The research presented in this paper focuses on the exploration of the d-wave gap in electron-doped Sr2IrO4 and its potential implications for high-temperature superconductivity (HTSC). This investigation is particularly notable as it parallels the properties of HTSC cuprates, offering a fresh perspective on the relationship between superconductivity and pseudogap phases.
Employing angle-resolved photoemission spectroscopy (ARPES), the paper investigates the low-temperature phase of electron-doped Sr2IrO4 with electron doping levels around 6-8%. Notably, the research identifies a d-wave symmetry in the gap, revealing gapless excitations at four isolated Brillouin zone points—a haLLMark of cuprate phenomenology. This significant finding confirms that Sr2IrO4 can reproduce the dual-phase characteristics observed in cuprates, specifically the transition from Fermi arcs to d-wave nodes.
The electron-doped Sr2IrO4 demonstrates a nodal Fermi surface at low temperatures, undetectable from single-electron band structure predictions. This behavior suggests a complex, correlated electronic phase arising from electron doping in Sr2IrO4. The density-functional predictions of a circular Fermi surface at the Γ point, consistent with earlier observations at higher temperatures and doping levels, complement these findings.
Temperature-dependent measurements of the gap indicate a k-dependence, with the gap magnitude extending up to approximately 22 meV at 10 K, yet absent at the node, contrasting with antinode behavior. The observed nodal metal phase seems dissociated from any phase transition. This aligns with the behavior of superconducting and non-superconducting cuprates, where near-nodal gaps emerge without explicit phase transitions, potentially linked to d-wave pairing correlations or a yet unidentified phase.
A crucial finding of this research is the heterogeneity in the gap profile, displaying larger gaps at the antinode compared to the d-wave form-derived near-nodal gaps. This indicates potentially distinct origins for the two gaps, perhaps elucidating the pseudogap's relation with superconducting gaps—a long-standing question in HTSC research.
Methodologically, the paper overcame challenges in achieving clean electron doping by employing in situ potassium deposition for surface electron doping, eschewing the typical challenges associated with chemical doping in Sr2IrO4. Additionally, the research used a material engineering approach by embedding Sr2IrO4 into Sr3Ir2O7, enhancing ARPES measurement capabilities at low temperatures without sample charging issues.
In conclusion, the paper establishes Sr2IrO4 as a promising non-cuprate platform for investigating the connection between pseudogap and d-wave superconducting gaps. Future work may focus on chemically doping the sample to verify the potential superconducting origin of these observations or uncover alternative quantum states that emerge, broadening our understanding of HTSC mechanisms in 5d transition-metal oxides. The implications extend to developing a comprehensive theory of HTSC, emphasizing the critical role of d-wave symmetry in high-temperature superconductors.