



@article {2316,
	title = {Quantum field theory for the chiral clock transition in one spatial dimension},
	journal = {Phys. Rev. },
	volume = {B },
	year = {2018},
	month = {2018/11/09},
	pages = {205118 },
	abstract = {<p>We describe the quantum phase transition in the N-state chiral clock model in spatial dimension d=1. With couplings chosen to preserve time-reversal and spatial inversion symmetries, such a model is in the universality class of recent experimental studies of the ordering of pumped Rydberg states in a one-dimensional chain of trapped ultracold alkali atoms. For such couplings and N=3, the clock model is expected to have a direct phase transition from a gapped phase with a broken global ZN symmetry, to a gapped phase with the ZN symmetry restored. The transition has dynamical critical exponent z\&ne;1, and so cannot be described by a relativistic quantum field theory. We use a lattice duality transformation to map the transition onto that of a Bose gas in d=1, involving the onset of a single boson condensate in the background of a higher-dimensional N-boson condensate. We present a renormalization group analysis of the strongly coupled field theory for the Bose gas transition in an expansion in 2\&minus;d, with 4\&minus;N chosen to be of order 2\&minus;d. At two-loop order, we find a regime of parameters with a renormalization group fixed point which can describe a direct phase transition. We also present numerical density-matrix renormalization group studies of lattice chiral clock and Bose gas models for N=3, finding good evidence for a direct phase transition, and obtain estimates for z and the correlation length exponent ν.</p>},
	doi = {https://doi.org/10.1103/PhysRevB.98.205118},
	url = {https://arxiv.org/abs/1808.07056},
	author = {Seth Whitsitt and Rhine Samajdar and Subir Sachdev}
}
