Spin-Singlet to Spin Polarized Phase Transition at : Flux-Trading in Action
arXiv:cond-mat/9507016 · doi:10.1016/0550-3213(95)00519-X
Abstract
We analyze the phase transition between spin-singlet and spin-polarized states which occurs at . The basic strategy is to use adiabatic flux-trading arguments to relate this transition to the analogous transition at . The transition is found to be similar to a transition in ferromagnets. In our analysis, we find two possible scenarios. In one, the transition is first-order, in agreement with experimental and numerical studies of the transition. In the other, we find a second-order transition to a partially polarized state followed by a second-order transition to a fully polarized state. This picture is in qualitative agreement with experiments on the state, the particle-hole conjugate of . We analyze the edge modes which propagate at the boundaries between regions of different phases and show that these do not support gapless excitations. Finally, we consider the possibility of a finite-temperature compressible state with a Fermi surface which would explain the non-zero seen in experiments.
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