The edge of a two-dimensional electron system in a magnetic field consists
of one-dimensional channels that arise from the confining electric field at
the edge of the system(1-3). The crossed electric and magnetic fields caus
e electrons to drift parallel to the sample boundary, creating a chiral cur
rent that travels along the edge in only one direction. In an ideal two-dim
ensional electron system in the quantum Hall regime, all the current flows
along the edge(4-6). Quantization of the Hall resistance arises from occupa
tion of N one-dimensional edge channels, each contributing a conductance of
e(2)/h (refs 7-11), Here we report differential conductance measurements,
in the integer quantum Hall regime, of tunnelling between the edges of a pa
ir of two-dimensional electron systems that are separated by an atomically
precise, high-quality, tunnel barrier. The resultant interaction between th
e edge states leads to the formation of new energy gaps and an intriguing d
ispersion relation for electrons travelling along the barrier: for example,
we see a persistent conductance peak at zero bias voltage and an absence o
f tunnelling features due to electron spin, These features are unexpected a
nd are not consistent with a model of weakly interacting edge states, Remna
nt disorder along the barrier and charge screening may each play a role, al
though detailed numerical studies will be required to elucidate these effec
ts.