Yuan Li

collaborators

5 papers

cond-mat.supr-con2026

Enhancement of $J$ $_{c}$ by Proton Irradiation in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8}$ $_{+}$ $_{I^} ´$ Single Crystals

Wenjie Li, Ran Guo, Xin Zhou +10

Critical current density is the key parameter for the practical application of superconductivity. In this study, 3 MeV proton irradiation experiments were conducted on HgBa $_{2}$ Ca$_…

cond-mat.supr-con2025

Strain-induced structural change and nearly-commensurate diffuse scattering in the model high-temperature superconductor HgBa $_{2}$ CuO $_{4 + I^´}$

Mai Ye, Wenshan Hong, Tom Lacmann +9

We investigate the strain response of underdoped HgBa $_{2}$ CuO $_{4 + I^´}$ (Hg1201), by synchrotron X-ray diffraction and corresponding simulations of thermal diffuse scattering. The co…

cond-mat.supr-con2025

Dominant apical-oxygen electron-phonon coupling in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8 + I^´}$

Wenshan Hong, Qizhi Li, Shilong Zhang +14

How electron-phonon interactions influence high-temperature superconductivity in cuprates remains contested, and their role outside the CuO $_{2}$ planes has been largely overlooked.…

cond-mat.supr-con2025

Unprecedentedly large gap in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8 + I^´}$ with the highest $T_{c}$ at ambient pressure

Chuanhao Wen, Zhiyong Hou, Alireza Akbari +6

In cuprate superconductors, the highest $T_{c}$ is possessed by the HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8 + I^´}$ (Hg-1223) system at ambient pressure, but the reason remains elusive. Here we repor…

cond-mat.supr-con2025

Three Magnetization Peaks in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8}$ Single Crystals

Yongze Ye, Yuhao Liu, Wenshan Hong +2

By measuring magnetization hysteresis loops of the superconducting HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8}$ single crystals ( $T_{c}$ = 133 K), we observed three magnetization peaks in a wide…

Enhancement of Jc​ by Proton Irradiation in HgBa2​Ca2​Cu3​O8​+​I^​´ Single Crystals

Strain-induced structural change and nearly-commensurate diffuse scattering in the model high-temperature superconductor HgBa2​CuO4+I^´​

Dominant apical-oxygen electron-phonon coupling in HgBa2​Ca2​Cu3​O8+I^´​

Unprecedentedly large gap in HgBa2​Ca2​Cu3​O8+I^´​ with the highest Tc​ at ambient pressure

Three Magnetization Peaks in HgBa2​Ca2​Cu3​O8​ Single Crystals

Enhancement of $J$ $_{c}$ by Proton Irradiation in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8}$ $_{+}$ $_{I^} ´$ Single Crystals

Strain-induced structural change and nearly-commensurate diffuse scattering in the model high-temperature superconductor HgBa $_{2}$ CuO $_{4 + I^´}$

Dominant apical-oxygen electron-phonon coupling in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8 + I^´}$

Unprecedentedly large gap in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8 + I^´}$ with the highest $T_{c}$ at ambient pressure

Three Magnetization Peaks in HgBa $_{2}$ Ca $_{2}$ Cu $_{3}$ O $_{8}$ Single Crystals