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A modest in-plane magnetic field Bpar is sufficient to destroy the fractional quantized Hall states at $ u = 5/2$ and 7/2 and replace them with anisotropic compressible phases. Remarkably, we find that at larger Bpar these anisotropic phases can themselves be replaced by isotropic compressible phases reminiscent of the composite fermion fluid at $ u = 1/2$. We present strong evidence that this transition is a consequence of the mixing of Landau levels from different electric subbands. We also report surprising dependences of the energy gaps at $ u = 5/2$ and 7/3 on the width of the confinement potential.
Under hydrostatic pressure, the ground state of a two-dimensional electron gas at $ u=5/2$ changes from a fractional quantum Hall state to the stripe phase. By measuring the energy gap of the fractional quantum Hall state and of the onset temperature
We investigate the finite frequency noise of a quantum point contact at filling factor { u} = 5/2 using a weakly coupled resonant LC circuit as a detector. We show how one could spectroscopically address the fractional charged excitations inspecting
We study the nature of the u=5/2 quantum Hall state in wide quantum wells under the mixing of electronic subbands and Landau levels. We introduce a general method to analyze the Moore-Read Pfaffian state and its particle-hole conjugate, the anti-Pfa
We investigate the nature of the fractional quantum Hall (FQH) state at filling factor $ u=13/5$, and its particle-hole conjugate state at $12/5$, with the Coulomb interaction, and address the issue of possible competing states. Based on a large-scal
Supersymmetry, a symmetry between fermions and bosons, provides a promising extension of the standard model but is still lack of experimental evidence. Recently, the interest in supersymmetry arises in the condensed matter community owing to its pote