activity
20222026
collaborators

6 papers

cond-mat.mes-hall2026

Topological superconductivity of a two-dimensional electron gas at the (001) LaAlO\textsubscript{3}/SrTiO\textsubscript{3} interface

Piotr Żeberek, Paweł Wójcik

We investigate the emergence of topological superconductivity and Majorana zero modes in the two-dimensional electron gas formed at the LaAlO/SrTiO (001) interface. Using a…

cond-mat.supr-con2025

Interplay between altermagnetism and superconductivity in two dimensions: intertwined symmetries and singlet-triplet mixing

Kinga Jasiewicz, Paweł Wójcik, Michał Nowak +1

We study the interplay between altermagnetism and unconventional superconductivity for the case of two-dimensional square- and triangular-lattice systems. Our approach is based on…

quant-ph2025

Broad nonlocal spectrum in the Pb-InSb hybrid three terminals for potential realization of Kitaev chains

Guoan Li, Xiaofan Shi, Ruixuan Zhang +21

Hybrid superconductor-semiconductor(SC-SM) nanowires remain one of the foremost platforms for engineering topological superconductivity and Majorana zero modes(MZMs) towards fault-…

cond-mat.mes-hall2025

Enhanced and modulable induced superconducting gap and effective Landé g-factor in Pb-InSb hybrid devices

Guoan Li, Xiaofan Shi, Ziwei Dou +21

The hybrid system of a conventional superconductor (SC) on a semiconductor (SM) nanowire with strong spin-orbit coupling (SOC) represents a promising platform for achieving topolog…

cond-mat.str-el2024

Variational Monte-Carlo Approach for Hubbard Model Applied to Twisted Bilayer WSe at Half-Filling

Andrzej Biborski, Paweł Wójcik, Michał Zegrodnik

We consider an effective Hubbard model with spin- and direction-dependent complex hoppings , applied to twisted homobilayer WSe using a variational Monte Carlo approach. The…

math.FA2022

An orthogonality relation in complex normed spaces based on norm derivatives

S. M. Enderami, M. Abtahi, A. Zamani +1

Let be a complex normed space. Based on the right norm derivative , we define a mapping by \begin{equation*} ρ_{_{\infty}}(x,y) = \frac1π\int_0^{2π}e^…