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- W1972502563 abstract "When the magnetic field is not aligned along one of the crystallographic axes of a quasi-1D conductor, the electronic motion is periodic only for special values of the field orientation. For these values, a cascade of spin-density-wave subphases is expected as the field increases. In each subphase the Hall resistance per layer is ${ensuremath{rho}}_{mathrm{xy}}=frac{mathrm{qh}}{p{e}^{2}}$. $q$ depends on the orientation of the field and $p$ on its amplitude. The electron motion involves large orbits which spread over $q$ unit cells. The integer quantization of these orbits implies a fractional quantization of the density of carriers." @default.
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- W1972502563 date "1989-02-20" @default.
- W1972502563 modified "2023-10-09" @default.
- W1972502563 title "Fractional Quantized Hall Effect in a Quasi-One-Dimensional Conductor" @default.
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- W1972502563 doi "https://doi.org/10.1103/physrevlett.62.953" @default.
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