材料科学

量子材料聚焦:KTaO3二维界面超导

  • 尹鑫茂 ,
  • 孙孟霞 ,
  • 宁苑杰 ,
  • 代靓 ,
  • 李敏娟 ,
  • 蔡传兵
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  • 上海大学 理学院 上海市高温超导重点实验室, 上海 200444

收稿日期: 2024-03-11

  网络出版日期: 2025-09-16

基金资助

国家自然科学基金资助项目(52172271, 12374378, 52307026); 国家重点研发计划资助项目(2022YFE03150200); 上海市科技创新行动计划资助项目(22511100200, 23511101600); 中科院先导专项(XDB25000000)

Focus on quantum materials: KTaO3 two-dimensional interface superconductivity

  • YIN Xinmao ,
  • SUN Mengxia ,
  • NING Yuanjie ,
  • DAI Liang ,
  • LI Minjuan ,
  • CAI Chuanbing
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  • Shanghai Key Laboratory of High Temperature Superconductors, College of Sciences, Shanghai University, Shanghai 200444, China

Received date: 2024-03-11

  Online published: 2025-09-16

摘要

钙钛矿氧化物异质界面中二维电子气(two-dimensionalelectron gas,2DEG)与界面超导性的发现使其成为研究热点之一.近年来,氧化物界面研究取得突破性进展,除了传统的LaAlO$_{3}$/SrTiO$_{3}$(LAO/STO)界面,2021年在KTaO$_{3}$(KTO)界面也发现超导性,其超导转变温度($T_{\rm c}$)较LAO/STO高出一个数量级,约为2 K,引起广泛关注.与STO界面体系相比,KTO氧化物界面显现出高载流子迁移率、强自旋轨道耦合(spin-orbit coupling,SOC)等特点,为理解非常规超导机制和构建新物理特性的研究提供了新途径,使KTO异质界面成为未来电子和自旋电子应用的有力候选者.本文旨在总结近5年KTO界面的最新进展,概述多种氧化物与KTO界面超导的新奇物理现象,并讨论目前研究中尚未解决的问题,为未来研究提供参考.

本文引用格式

尹鑫茂 , 孙孟霞 , 宁苑杰 , 代靓 , 李敏娟 , 蔡传兵 . 量子材料聚焦:KTaO3二维界面超导[J]. 上海大学学报(自然科学版), 2025 , 31(4) : 591 -606 . DOI: 10.12066/j.issn.1007-2861.2582

Abstract

The discovery of two-dimensional electron gas (2DEG) and interfacial superconductivity within perovskite oxide heterostructures has made them one of the research hotspots. In recent years, there have been groundbreaking advancements in the study of oxide interfaces. In addition to the conventional LaAlO$_{3}$/SrTiO$_{3}$ (LAO/STO) interface, superconductivity has been observed at the KTaO$_{3}$ (KTO) interface in 2021, with a superconducting transition temperature ($T_{\rm c}$) approximately an order of magnitude higher than that of LAO/STO, reaching around 2 K, sparking widespread attention. Compared to the STO interface system, the KTO oxide interface exhibits characteristics such as high carrier mobility and strong spin-orbit coupling (SOC), providing a new avenue for understanding the mechanism of unconventional superconductivity and studying new physical properties, thus establishing KTO heterostructures as promising candidates for future electronic and spintronic applications. This paper aims to summarize the latest progress in KTO interfaces over the past five years, provide an in-depth overview of the novel physical phenomena of superconductivity at the interfaces of various oxides and KTO, and discuss unresolved issues in current researches, thereby guiding the direction of future investigations.

参考文献

[1] Reyren N, Thiel S, Caviglia A D, et al. Superconducting interfaces between insulating oxides [J]. Science, 2007, 317(5842): 1196-1199.
[2] Gozar A, Logvenov G, Kourkoutis L F, et al. High-temperature interface superconductivity between metallic and insulating copper oxides [J]. Nature, 2008, 455(7214): 782-785.
[3] Li D, Lee K, Wang B Y, et al. Superconductivity in an inflnite-layer nickelate [J]. Nature, 2019, 572(7771): 624-627.
[4] Ugeda M M, Bradley A J, Zhang Y, et al. Characterization of collective ground states in single-layer NbSe2 [J]. Nature Physics, 2015, 12(1): 92-97.
[5] Cao Y, Fatemi V, Fang S, et al. Unconventional superconductivity in magic-angle graphene superlattices [J]. Nature, 2018, 556(7699): 43-50.
[6] Chen G, Sharpe A L, Gallagher P, et al. Signatures of tunable superconductivity in a trilayer graphene moire superlattice [J]. Nature, 2019, 572(7768): 215-219.
[7] Liu Y, Ma C, Zhang Q, et al. 2D electron gas and oxygen vacancy induced high oxygen evolution performances for advanced Co3O4/CeO2 nanohybrids [J]. Advanced Materials, 2019, 31(21): 1900062.
[8] Chen Y Z, Bovet N, Trier F, et al. A high-mobility two-dimensional electron gas at the spinel/perovskite interface of γ-Al2O3/SrTiO3 [J]. Nature Communications, 2013, 4(1): 1371.
[9] He T, Liu W, Lv T, et al. MXene/SnO2 heterojunction based chemical gas sensors [J]. Sensors and Actuators B: Chemical, 2021, 329: 129275.
[10] Bert J A, Kalisky B, Bell C, et al. Direct imaging of the coexistence of ferromagnetism and superconductivity at the LaAlO3/SrTiO3 interface [J]. Nature Physics, 2011, 7(10): 767-771.
[11] Caviglia A D, Gariglio S, Reyren N, et al. Electric fleld control of the LaAlO3/SrTiO3 interface ground state [J]. Nature, 2008, 456(7222): 624-627.
[12] Tang C S, Zeng S, Diao C, et al. Two-dimensional charge localization at the perovskite oxide interface [J]. Applied Physics Reviews, 2022, 9(3): 031405.
[13] Edge J M, Kedem Y, Aschauer U, et al. Quantum critical origin of the superconducting dome in SrTiO3 [J]. Physical Review Letters, 2015, 115(24): 247002.
[14] Richter C, Boschker H, Dietsche W, et al. Interface superconductor with gap behaviour like a high-temperature superconductor [J]. Nature, 2013, 502(7472): 528-531.
[15] Liu C, Yan X, Jin D, et al. Two-dimensional superconductivity and anisotropic transport at KTaO3(111) interfaces [J]. Science, 2021, 371(6530): 716-721.
[16] Thompson J R, Boatner L A, Thomson J O. Very low-temperature search for superconductivity in semiconducting KTaO3 [J]. Journal of Low Temperature Physics, 1982, 47(5): 467-475.
[17] Chen Z, Liu Y, Zhang H, et al. Electric fleld control of superconductivity at the LaAlO3/KTaO3(111) interface [J]. Science, 2021, 372(6543): 721-724.
[18] Cooper V R. Enhanced carrier mobilities in two-dimensional electron gases at III-III/I-V oxide heterostructure interfaces [J]. Physical Review B, 2012, 85(23): 235109.
[19] Himmetoglu B, Janotti A. Transport properties of KTaO3 from flrst-principles [J]. Journal of Physics: Condensed Matter, 2016, 28(6): 065502.
[20] Zhang H, Yun Y, Zhang X, et al. High-mobility spin-polarized two-dimensional electron gases at EuO/KTaO3 interfaces [J]. Physical Review Letters, 2018, 121(11): 116803.
[21] Goyal S, Wadehra N, Chakraverty S. Tuning the electrical state of 2DEG at LaVO3iKTaO3 interface: efiect of light and electrostatic gate [J]. Advanced Materials Interfaces, 2020, 7(16): 2000646.
[22] Jellison G E, Paulauskas I, Boatner L A, et al. Optical functions of KTaO3 as determined by spectroscopic ellipsometry and comparison with band structure calculations [J]. Physical Review B, 2006, 74(15): 155130.
[23] Fujiwara T, Sasahara A, Happo N, et al. Single-crystal model of highly e-cient watersplitting photocatalysts: a KTaO3 wafer doped with calcium cations [J]. Chemistry of Materials, 2020, 32(4): 1439-1447.
[24] Wadehra N, Tomar R, Halder S, et al. Electronic structure modiflcation of the KTaO3 single-crystal surface by Ar+ bombardment [J]. Physical Review B, 2017, 96(11): 115423.
[25] King P D, He R H, Eknapakul T, et al. Subband structure of a two-dimensional electron gas formed at the polar surface of the strong spin-orbit perovskite KTaO3 [J]. Physical Review Letters, 2012, 108(11): 117602.
[26] Tyunina M, Narkilahti J, Plekh M, et al. Evidence for strain-induced ferroelectric order in epitaxial thin-fllm KTaO3 [J]. Physical Review Letters, 2010, 104(22): 227601.
[27] Bae I T, Ichinose T, Han M G, et al. Tensile stress efiect on epitaxial BiFeO3 thin fllm grown on KTaO3 [J]. Scientiflc Reports, 2018, 8(1): 893.
[28] Golovina I S, Kolesnik S P, Bryksa V P, et al. Defect driven ferroelectricity and magnetism in nanocrystalline KTaO3 [J]. Physica B: Condensed Matter, 2012, 407(4): 614-623.
[29] Sakai A, Kanno T, Yotsuhashi S, et al. Thermoelectric properties of electron-doped KTaO3 [J]. Japanese Journal of Applied Physics, 2009, 48(9): 097002.
[30] Yamaichi E, Watanabe K, Imamiya K, et al. Photoluminescence in KTaO3 single crystal [J]. Journal of the Physical Society of Japan, 1987, 56(5): 1890-1897.
[31] Zhou Z, Huang G, Shen J, et al. WSe2/2D electron gas heterojunction on KTaO3 for roomtemperature giant photoconductivity [J]. Ceramics International, 2021, 47(6): 7425-7429.
[32] Dumen M, Singh A, Goyal S, et al. Photoconductivity of the EuO KTO interface: efiect of intrinsic carrier density and temperature [J]. The Journal of Physical Chemistry C, 2021, 125(28): 15510-15515.
[33] Chen Z, Liu Z, Sun Y, et al. Two-dimensional superconductivity at the LaAlO3/KTaO3(110) heterointerface [J]. Physical Review Letters, 2021, 126(2): 026802.
[34] Nakamura H, Kimura T. Electric fleld tuning of spin-orbit coupling in KTaO3 fleld-efiect transistors [J]. Physical Review B, 2009, 80(12): 121308.
[35] Gariglio S, Caviglia A D, Triscone J M, et al. A spin-orbit playground: surfaces and interfaces of transition metal oxides [J]. Reports on Progress in Physics, 2019, 82(1): 012501.
[36] Hua X, Meng F, Huang Z, et al. Tunable two-dimensional superconductivity and spin-orbit coupling at the EuO/KTaO3(110) interface [J]. NPJ Quantum Materials, 2022, 7(1): 97.
[37] Hua X, Zeng Z, Meng F, et al. Superconducting stripes induced by ferromagnetic proximity in an oxide heterostructure [J]. Nature Physics, 2024, 20(6): 957-963.
[38] Qiao W, Ma Y, Yan J, et al. Gate tunability of the superconducting state at the EuO/KTaO3(111) interface [J]. Physical Review B, 2021, 104(18): 184505.
[39] Liu C, Zhou X, Hong D, et al. Tunable superconductivity and its origin at KTaO3 interfaces [J]. Nature Communications, 2023, 14: 951.
[40] Sun Y, Liu Y, Hong S, et al. Critical thickness in superconducting LaAlO3/KTaO3(111) heterostructures [J]. Physical Review Letters, 2021, 127(8): 086804.
[41] Chen X, Yu T, Liu Y, et al. Orientation-dependent electron-phonon coupling in interfacial superconductors LaAlO3/KTaO3 [DB/OL]. (2023-01-31) [2024-02-20]. http://arxiv.org/abs/2301.13488.
[42] Mallik S, Menard G C, Saiz G, et al. Superfluid stifiness of a KTaO3-based two-dimensional electron gas [J]. Nature Communications, 2022, 13: 4625.
[43] Al-Tawhid A H, Kanter J, Hatefipour M, et al. Superconductivity and weak antilocalization at KTaO3(111) interfaces [J]. Journal of Electronic Materials, 2022, 51(11): 6305- 6309.
[44] Liu Y, Liu Z, Zhang M, et al. Superconductivity in epitaxially grown LaVO3/KTaO3(111) heterostructures [J]. Chinese Physics B, 2023, 32(3): 037305
[45] Maryenko D, Maznichenko I V, Ostanin S, et al. Superconductivity at epitaxial LaTiO3- KTaO3 interfaces [J]. APL Materials, 2023, 11(6): 061102.
[46] Kim J, Yu M, Lee J-W, et al. Electronic-grade epitaxial (111) KTaO3 heterostructures [J]. Science Advances, 2024, 10(21): eadk4288.
[47] Arnault EG, Al-Tawhid A H, Salmani-Rezaie S, et al. Anisotropic superconductivity at KTaO3(111) interfaces [J]. Science Advances, 2023, 9(7): eadf1414.
[48] Gan Y, Yang F, Kong L, et al. Light-induced giant rashba spin-orbit coupling at superconducting KTaO3(110) heterointerfaces [J]. Advanced Materials, 2023, 35(25): 2370180.
[49] Al-Tawhid A H, Poage S J, Salmani-Rezaie S, et al. Enhanced critical fleld of superconductivity at an oxide interface [J]. Nano Letters, 2023, 23(15): 6944-6950.
[50] Zhang G, Wang L, Wang J, et al. Spontaneous rotational symmetry breaking in KTaO3 heterointerface superconductors [J]. Nature Communications, 2023, 14: 3046.
[51] Ueno K, Inoue I H, Yamada T, et al. Field-efiect transistor based on KTaO3 perovskite [J]. Applied Physics Letters, 2004, 84(19): 3726-3728.
[52] Sekiya D, Nakamura H, Kimura T. Enhanced carrier injection in perovskite fleld-efiect transistors via low-barrier contacts [J]. Applied Physics Express, 2011, 4(6): 064103.
[53] Zhang C, Zhang X, Xu R, et al. Ion-liquid-gated KTaO3-based electric double layer transistor [J]. IEEE Electron Device Letters, 2023, 44(12): 1987-1990.
[54] Tian X, Li B, Sun H, et al. Visible-light-driven semiconductor-metal transition in electron gas at the (100) surface of KTaO3 [J]. Nanomaterials, 2023, 13(23): 3055.
[55] Goyal S, Tomar R, Chakraverty S. Photodynamics study of KTaO3-based conducting interfaces [J]. ACS Applied Electronic Materials, 2021, 3(2): 905-911.
[56] Zhai J, Trama M, Liu H, et al. Large nonlinear transverse conductivity and berry curvature in KTaO3 based two-dimensional electron gas [J]. Nano Letters, 2023, 23(24): 11892-11898.
[57] Kumar N, Kakkar S, Bera C. High thermoelectric power factor in LaVO3/KTaO3 heterostructure [J]. Physica E: Low-Dimensional Systems and Nanostructures, 2023, 146: 115525.
[58] Ojha S K, Gogoi S K, Patidar M M, et al. Oxygen vacancy-induced topological Hall efiect in a nonmagnetic band insulator [J]. Advanced Quantum Technologies, 2020, 3(7): 2000021.
[59] Wadehra N, Chakraverty S. Electrostatic memory in KTaO3 [J]. Applied Physics Letters, 2019, 114(16): 163103.
[60] Zhang H, Zhu Z, Zhu Y C, et al. Fermi-level-dependent charge-to-spin conversion of the twodimensional electron gas at the γ-Al2O3/KTaO3 interface [J]. Physical Review Applied, 2023, 19(3): 034045.
[61] Zheng S, Ma J, Fang K, et al. High-voltage potassium ion micro-supercapacitors with extraordinary volumetric energy density for wearable pressure sensor system [J]. Advanced Energy Materials, 2021, 11(17): 2003835.
[62] Garcia-Barcelo J M, Melcon A A, Cuendis S A, et al. On the development of new tuning and inter-coupling techniques using ferroelectric materials in the detection of dark matter axions [J]. IEEE Access, 2023, 11: 30360-30372.
[63] Kumar N, Wadehra N, Tomar R, et al. Observation of Shubnikov de Haas oscillations, planar Hall efiect, and anisotropic magnetoresistance at the conducting interface of EuO KTaO3 [J]. Advanced Quantum Technologies, 2020, 4(1): 2000081.
[64] Zhang H, Ma Y, Zhang H, et al. Thermal spin injection and inverse edelstein efiect of the twodimensional electron gas at EuO-KTaO3 interfaces [J]. Nano Letters, 2019, 19(3): 1605-1612.
[65] Ren T, Li M, Sun X, et al. Two-dimensional superconductivity at the surfaces of KTaO3 gated with ionic liquid [J]. Science Advances, 2022, 8(22): eabn4273.
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