  Graphene is a stable single atomic layer material exhibiting two-dimensional
electron gas of massless Dirac fermions of high mobility. One of the intriguing
properties of graphene is a possibility of realization of the Tamm-type edge
states. These states differ from the usual surface states caused by defects,
impurities and other imperfections at the edge of the system, as well as they
differ from the magnetic edge states caused by skipping cyclotron orbits. The
Tamm states result from breaking of periodic crystal potential at the edge,
they can exist even at zero magnetic field and form a conducting band. Until
recently those states have been observed in graphene only by local STM
technique and there were no direct experiments on their contribution to
transport measurements. Here we present the experiments on Aharonov-Bohm (AB)
oscillations of resistance in a single-nanohole graphite and graphene
structures, it indicates the presence of conducting edge states cycling around
nanohole. An estimation show the penetration depth of the edge states to be as
short as about 2 nm. The oscillations persist up to temperature T=115 K and the
T-range of their existence increases with a decrease of the nanohole diameter.
The proposed mechanism of the AB oscillations based on the resonant intervalley
backscattering of the Dirac fermions by the nanohole via the Tamm states. The
experimental results are consistent with such a scenario. Our findings show a
way towards interference devices operating at high temperatures on the edge
states in graphene
