Quantum disordered phase in a doped antiferromagnet
arXiv:cond-mat/9407112 · doi:10.1016/0921-4534(94)92346-9
Abstract
A quantitative description of the transition to a quantum disordered phase in a doped antiferromagnet is obtained with a U(1) gauge-theory, where the gap in the spin-wave spectrum determines the strength of the gauge-fields. They mediate an attractive long-range interaction whose possible bound-states correspond to charge-spin separation and pairing.
11 pages, LaTex, chris-preprint-1994-1