# Evolution of ferromagnetism in two-dimensional electron gas of LaTiO3/SrTiO3

## TL;DR

This paper investigates the magnetic properties of a two-dimensional electron gas at LaTiO3/SrTiO3 interfaces, revealing magnetic phase separation and spin polarization, which are crucial for spintronics applications.

## Contribution

It provides experimental evidence of magnetic phase separation and spin polarization in LaTiO3/SrTiO3 2DEG, highlighting the role of magnetic instabilities in doped Mott insulators.

## Key findings

- Evidence for magnetic phase separation in hole-doped Ti system
- Observation of hysteresis indicating spin-polarized magnetic islands
- Role of magnetic instabilities in doped Mott insulators

## Abstract

Understanding, creating, and manipulating spin polarization of two-dimensional electron gases at complex oxide interfaces presents an experimental challenge. For example, despite almost a decade long research effort, the microscopic origin of ferromagnetism in LaAlO3/SrTiO3 heterojunction is still an open question. Here, by using a prototypical two-dimensional electron gas (2DEG) which emerges at the interface between band insulator SrTiO3 and antiferromagnetic Mott insulator LaTiO3 , the experiment reveals the evidence for magnetic phase separation in hole-doped Ti d1 t2g system resulting in spin-polarized 2DEG. The details of electronic and magnetic properties of the 2DEG were investigated by temperature-dependent d.c. transport, angle-dependent X-ray photoemission spectroscopy, and temperature-dependent magnetoresistance. The observation of clear hysteresis in magnetotransport at low magnetic fields implies spin-polarization from magnetic islands in the hole rich LaTiO3 near the interface. These findings emphasize the role of magnetic instabilities in doped Mott insulators thus providing another path for designing all-oxide structures relevant to spintronics applications.