Spin-squeezed Ground States in the Bilayer Quantum Hall Ferromagnet

Details Spin-squeezed Ground States in the Bilayer Quantum Hall Ferromagnet Spin-squeezed Ground States in the Bilayer Quantum Hall Ferromagnet

1997-11-05

arxiv.org/abs/cond-mat/9711030v1

Physics

Condensed Matter

Mesoscale and Nanoscale Physics

4 pages, revtex, one figure, to appear in PRB Rapid Communication

Scientific paper

10.1103/PhysRevB.56.R15549

A "squeezed-vacuum" state considered in quantum optics is shown to be realized in the ground-state wavefunction for the bilayer quantum Hall system at the total Landau level filling of $\nu=1/m$ (m: odd integer). This is derived in the boson approximation, where a particle-hole pair creation across the symmetric-antisymmetric gap, $\Delta_{SAS}$, is regarded as a boson. In terms of the pseudospin describing the layers, the state is a spin-squeezed state, where the degree of squeezing is controlled by the layer separation and $\Delta_{SAS}$. An exciton condensation, which amounts to a rotated spin-squeezed state, has a higher energy due to the degraded SU(2) symmetry for $\Delta_{SAS} \neq 0$.

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