Group V element analogues of graphene have attracted a lot attention recently due to their semiconducting band structures, which make them promising for next generation electronic and optoelectronic devices based on two-dimensional materials. Theoretical investigations predict high electron mobility, large band gaps, band gap tuning by strain, formation of topological phases, quantum spin Hall effect at room temperature, and superconductivity amongst others. Here, we report a successful formation of freestanding like monolayer arsenene on Ag(111). This was concluded from our experimental atomic and electronic structure data by comparing to results of our theoretical calculations. Arsenene forms a buckled honeycomb layer on Ag(111) with a lattice constant of 3.6 Å showing an indirect band gap of ~1.4 eV as deduced from the position of the Fermi level pinning.The isolation of two-dimensional (2D) carbon in the form of a single layer honeycomb structure (graphene) 1 was the starting point of today's intensive research on various 2D materials. In particular, the electronic properties, i.e., the high conductivity in combination with the linear dispersion of the -band, forming a Dirac cone, are highly interesting for applications in nanoelectronics 2 . However, this utilization of graphene is severely hampered by the lack of an intrinsic band gap, which it shares with graphene like structures of other group IV atoms, i.e., Si, Ge, and Sn 3 .