Quantum Hall system in Tao-Thouless limit

We consider spin-polarized electrons in a single Landau level on a torus. The quantum Hall problem is mapped onto a one-dimensional lattice model with lattice constant $2\pi /L_1$, where $L_1$ is a circumference of the torus (in units of the magnetic length). In the Tao-Thouless limit $L_1\to 0$, the interacting many-electron problem is exactly diagonalized at any rational filling factor $\nu =p/q\le 1$. For odd $q$, the ground state has the same qualitative properties as a bulk $\left(L_1\to \infty \right)$ quantum Hall hierarchy state and the lowest-energy quasiparticle excitations have the same fractional charges as in the bulk. These states are the $L_1\to 0$ limits of the Laughlin and Jain wave functions for filling fractions where these exist. We argue that the exact solutions generically, for odd $q$, are continuously connected to the two-dimensional bulk quantum Hall hierarchy states—i.e., that there is no phase transition as $L_1\to \infty$ for filling factors where such states can be observed. For even-denominator fractions, a phase transition occurs as $L_1$ increases. For $\nu =1/2$ this leads to the system being mapped onto a Luttinger liquid of neutral particles at small but finite $L_1$; this then develops continuously into the composite fermion wave function that is believed to describe the bulk $\nu =1/2$ system. The analysis generalizes to non-Abelian quantum Hall states.