Z. Huang

activity

20022021

most citedOrigin of the two-dimensional electron gas at LaAlO3/SrTiO3 interfaces: The role of oxygen vacancies and electronic reconstruction

219 citations · 721 across the 15 of their papers we have counts for

collaborators

Showing 2017Show all

5 papers · 1 filter

cond-mat.str-el2017★ 3 cited

Strong spin-orbit coupling and magnetism in (111) (La $_{0.3}$ Sr $_{0.7}$ )(Al $_{0.65}$ Ta $_{0.35})$ /SrTiO $_{3}$

V. V. Bal, Z. Huang, K. Han +3

Strong correlations, multiple lattice degrees of freedom, and the ease of doping make complex oxides a source of great research interest. Complex oxide heterointerfaces break inver…

cond-mat.str-el2017★ 9 cited

Signatures of Electronic Nematicity in (111) LaAlO $_{3}$ /SrTiO $_{3}$ Interfaces

S. Davis, Z. Huang, K. Han +3

Symmetry breaking is a fundamental concept in condensed matter physics whose presence often heralds new phases of matter. For instance, the breaking of time reversal symmetry is tr…

cond-mat.str-el2017★ 20 cited

Magnetoresistance in the superconducting state at the (111) LaAlO $_{3}$ /SrTiO $_{3}$ interface

S. Davis, Z. Huang, K. Han +3

Condensed matter systems that simultaneously exhibit superconductivity and ferromagnetism are rare due the antagonistic relationship between conventional spin-singlet superconducti…

cond-mat.str-el2017★ 6 cited

Electrostatic tuning of magnetism at the conducting (111) (La $_{0.3}$ Sr $_{0.7}$ )(Al $_{0.65}$ Ta $_{0.35}$ )/SrTiO $_{3}$ interface

V. V. Bal, Z. Huang, K. Han +3

We present measurements of the low temperature electrical transport properties of the two dimensional carrier gas that forms at the interface of $(111)$ (La $_{0.3}$ Sr $_{0.7}$ )(Al$_…

cond-mat.str-el2017★ 13 cited

Superconductivity and Frozen Electronic States at the (111) LaAlO $_{3}$ /SrTiO $_{3}$ Interface

S. Davis, Z. Huang, K. Han +3

In spite of Anderson's theorem, disorder is known to affect superconductivity in conventional s-wave superconductors. In most superconductors, the degree of disorder is fixed durin…

Strong spin-orbit coupling and magnetism in (111) (La0.3​Sr0.7​)(Al0.65​Ta0.35​)/SrTiO3​

Signatures of Electronic Nematicity in (111) LaAlO3​/SrTiO3​ Interfaces

Magnetoresistance in the superconducting state at the (111) LaAlO3​/SrTiO3​ interface

Electrostatic tuning of magnetism at the conducting (111) (La0.3​Sr0.7​)(Al0.65​Ta0.35​)/SrTiO3​ interface

Superconductivity and Frozen Electronic States at the (111) LaAlO3​/SrTiO3​ Interface

Strong spin-orbit coupling and magnetism in (111) (La $_{0.3}$ Sr $_{0.7}$ )(Al $_{0.65}$ Ta $_{0.35})$ /SrTiO $_{3}$

Signatures of Electronic Nematicity in (111) LaAlO $_{3}$ /SrTiO $_{3}$ Interfaces

Magnetoresistance in the superconducting state at the (111) LaAlO $_{3}$ /SrTiO $_{3}$ interface

Electrostatic tuning of magnetism at the conducting (111) (La $_{0.3}$ Sr $_{0.7}$ )(Al $_{0.65}$ Ta $_{0.35}$ )/SrTiO $_{3}$ interface

Superconductivity and Frozen Electronic States at the (111) LaAlO $_{3}$ /SrTiO $_{3}$ Interface