Spin-orbit-assisted electron pairing in one-dimensional waveguides

Abstract

Understanding and controlling the transport properties of interacting fermions is a key forefront in quantum physics across a variety of experimental platforms. Motivated by recent experiments in one-dimensional (1D) electron channels written on the LaAlO 3 /SrTiO 3 interface, we analyze how the presence of different forms of spin-orbit coupling (SOC) can enhance electron pairing in 1D waveguides. We first show how the intrinsic Rashba SOC felt by electrons at interfaces such as LaAlO 3 /SrTiO 3 can be reduced when they are confined in one dimension. Then, we discuss how SOC can be engineered, and show using a mean-field Hartree-Fock-Bogoliubov model that SOC can generate and enhance spin-singlet and -triplet electron pairing. Our results are consistent with two recent sets of experiments [Briggeman et al., Nat. Phys. 17, 782787 (2021); Sci. Adv. 6, eaba6337 (2020)] that are believed to engineer the forms of SOC investigated in this work, which suggests that metal-oxide heterostructures constitute attractive platforms to control the collective spin of electron bound states. However, our findings could also be applied to other experimental platforms involving spinful fermions with attractive interactions, such as cold atoms.

Possible zero-magnetic field fractional quantization in In0.75Ga0.25As heterostructures

“…If this changes to n 1 ¼ 1 and n 2 ¼ 3, then the increase to 0.4 Â (e 2 /h) follows. The subsequent decrease to 0.25 cannot be explained by this model and possibly points to a pairing which has been suggested can be a consequence of the RSOI 28 or found due to a repulsive potential. 29 A similar phenomenon has been reported in Ge, 1 where a 0.25 Â (e 2 /h) plateau is also observed when B // ¼ 8 T. However, the 0.25 Â (e 2 /h) originated from a 0.5 Â (e 2 /h) plateau at zero-field and was halved as a result of spin-polarization at a high field.…”