formed by edge states in the quantum Hall regime. The circuit consists of a wide Hall bar
(the inductor L) in series with a tunable resistor (R) formed by a quantum point contact.
Electron interactions between edges are screened by a pair of side gates. Conductance
steps are observed on both real and imaginary parts of the admittance. Remarkably, the
phase of the admittance is transmission independent. This shows that the relaxation time of …