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VOLUME 49 (1989) | ISSUE 11 | PAGE 628
Induced-spin confinement and high-temperature superconductivity
A condition for the quantization of induced spin in (2 + 1) -dimensional systems is derived. This condition is analogous to the Dirac condition for the quantization of magnetic charge. Particles whose induced spin is neither an integer nor a half-integer exist only in bound states. The superconducting phase differs from a spin liquid, which is presently being discussed in the context of high-temperature superconductivity.