超导材料和物理。

招收物理学、材料学、化学等专业研究生。

080501-材料物理与化学

超导薄膜材料和物理
低维超导材料研究

2005-09--2010-07   中国科学院物理研究所/中国科学院大学   理学博士学位
2001-09--2005-07   北京师范大学   学士学位

2020年- 今，  中科院上海微系统所，研究员

2012年-2019年，  中科院上海微系统所，副研究员

2010年-2012年，日本东北大学（Tohoku University），JSPS博士后

超导电子学-超导材料与物理基础

[1] Superconductivity above 30 K due to the introduction of oxygen in CaFeAsF. J. Mater. Chem. C 13, 1793 (2025).

[2] Coexistence of Ferromagnetism and Superconductivity at KTaO₃ Heterointerfaces. Nano Lett. 24, 7134−7141 (2024) .

[3] Microwave loss and kinetic inductance of epitaxial TiN films. Supercond. Sci. Technol. 37, 115002 (2024) . 

[4] From weak to strong-coupling superconductivity tuned by substrate in TiN films. Supercond. Sci. Technol. 37, 105015 (2024) . 

[5] Size effect on the response of superconductivity in NbN nanowires to external magnetic field. Supercond. Sci. Technol. 37, 085009 (2024).

[6] Investigation of the Pauli paramagnetic effect in systematically tuned NbN thin films. Physica C 606, 1354223 (2023). 

[7] Robust quantum Griffiths singularity above 1.5 K in nitride thin films. Phys. Rev. B 107, 094509 (2023).

[8] Two-Dimensional Superconductivity at the Titanium Sesquioxide Heterointerface. ACS Nano 16, 16150 (2022). (IF: 18.027)

[9] Universal relation between doping content and normal-state resistance in gate voltage tuned ultrathin Bi₂Sr₂CaCu₂O_8+x flakes. Phys. Rev. B 106, 104509 (2022). 

[10] Evolution of the upper critical field and superconducting vortex phase with thickness in PLD-grown Ta films. Supercond. Sci. Technol. 35, 055010 (2022). 

[11] Topological frequency shift of quantum oscillation in CaFeAsF. npj Quantum Mater. 7, 25 (2022). 

[12] Anomalous high-field magnetotransport in CaFeAsF due to the quantum Hall effect. npj Quantum Mater. 7, 62 (2022). 

[13] Direct Observation of the Topological Surface State in the Topological Superconductor 2M-WS₂. Nano Lett. 22, 8827 (2022). (IF: 12.262) 

[14] Discovery of Superconductivity in 2M WS₂ with Possible Topological Surface States. Adv. Mater. 31, 1901942 (2019). (IF: 25.809)

[15] Structure Re-determination and Superconductivity Observation of Bulk 1T MoS₂. Angew. Chem. Int. Ed. 57, 1232 (2018). (IF: 12.257)

[16] Low temperature specific heat of the hole-doped Ba_0.6K_0.4Fe₂As₂ single crystals. Phys. Rev. B 79, 174501 (2009). (Citations: 133)

[17] Nodal Gap in Fe-Based Layered Superconductor LaO_0.9F_0.1-δFeAs Probed by Specific Heat Measurements. Chin. Phys. Lett. 25, 2221 (2008).  (Citations: 135)

[18] Synthesis, structural, and transport properties of the hole-doped superconductor Pr_1-xSr_xFeAsO. Phys. Rev. B 79, 104501 (2009). (Citations: 30)

[19] Superconductivity at 25K in hole-doped (La_1−xSr_x)OFeAs. EPL, 82, 17009 (2008).  (Citations: 518)

[20] Strong Pauli paramagnetic effect in the upper critical field of KCa₂Fe₄As₄F₂. Sci. China-Phys. Mech. Astron. 63, 227412 (2020).

[21] Two-gap superconductivity in CaFe_0.88Co_0.12AsF revealed by temperature dependence of the lower critical field H_c1^c (T). npj Quantum Mater. 4, 33 (2019).

[22] Single-Crystal Growth and Extremely High H_c2 of 12442-Type Fe-Based Superconductor KCa₂Fe₄As₄F₂. J. Phys. Chem. C 123, 13925 (2019).

[23] Growth and characterization of CaFe_1-xCo_xAsF single crystals by CaAs flux method. J. Cryst. Growth, 451, 161 (2016).

[24] Growth and characterization of millimetersized single crystals of CaFeAsF. Supercond. Sci. Technol. 28, 085008 (2015)

[25] Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr_1-xSr_xFeAsO. Physica C 498, 50–53 (2014) 

[26] Anisotropic structure of the order parameter in FeSe_0.45Te_0.55 revealed by angle-resolved specific heat. Nat. Commun. 1, 112 (2010) 

[27] High-Tc superconductivity in ultrathin Bi₂Sr₂CaCu₂O_8+x down to half-unit-cell thickness by protection with graphene. Nat. Commun. 5, 5708 (2014) 

[28] Absence of Superconductivity in LiCu₂P₂. J. Am. Chem. Soc. 133, 1751–1753 (2011)