In common with other iron-based high temperature superconductors, FeSe exhibits a transition to a ``nematic'' phase below 90Kelvin in which the crystal rotation symmetry is spontaneously broken. However, the absence of strong low-frequency magnetic fluctuations near or above the transition has been interpreted as implying the primacy of orbital ordering. In contrast, we establish that quantum fluctuations of spin-1 local moments with strongly frustrated exchange interactions can lead to a nematic quantum paramagnetic phase consistent with the observations in FeSe. We show that this phase is a fundamental expression of the existence of a Berry's phase associated with the topological defects of a N\'eel antiferromagnet, in a manner analogous to that which gives rise to valence bond crystal order for spin 1/2 systems. We present an exactly solvable model realizing the nematic quantum paramagnetic phase, discuss its relation with the spin-1 J1−J2 model, and construct a field theory of the Landau-forbidden transition between the N\'eel state and this nematic quantum paramagnet.
@article{arxiv.1501.00844,
title = {Nematicity and quantum paramagnetism in FeSe},
author = {Fa Wang and Steven A. Kivelson and Dung-Hai Lee},
journal= {arXiv preprint arXiv:1501.00844},
year = {2015}
}