High field electron spin resonance, nuclear magnetic resonance and magnetization studies addressing the ground state of the quasi two-dimensional spin-1/2 honeycomb lattice compound InCu 2/3 V 1/3 O3 are reported. Uncorrelated finite size structural domains occurring in the honeycomb planes are expected to inhibit long range magnetic order. Surprisingly, ESR data reveal the development of two collinear antiferromagnetic (AFM) sublattices below ∼ 20 K whereas NMR results show the presence of the staggered internal field. Magnetization data evidence a spin reorientation transition at ∼ 5.7 T. Quantum Monte-Carlo calculations show that switching on the coupling between the honeycomb spin planes in a finite size cluster yields a Néel-like AFM spin structure with a substantial staggered magnetization at finite temperatures. This may explain the occurrence of a robust AFM state in InCu 2/3 V 1/3 O3 despite an unfavorable effect of structural disorder.PACS numbers: 75.50. Ee, 76.30.Fc, 75.10.Jm In planar honeycomb lattice systems a combination of nontrivial topology, strong electronic, spin and orbital correlations and degeneracies yields a rich variety of ground states, novel excitations and exotic behaviors that currently attract much attention. The recently discovered exciting phenomena range, e.g., from the quantum Hall effect in graphene 1,2 , superconductivity in MgB 2 3 and intercalated graphite 4 , to topologically driven quantum phase transitions in anyonic quantum liquids 5 .Regarding the spin degrees of freedom, an important feature of low dimensional spin systems is the presence of quantum fluctuations that inhibit long range order of the quantum spin-1/2 lattice. Such an effect essentially depends on the spin coordination number z. The one dimensional (1D) Heisenberg antiferromagnetic (AFM) S = 1/2 chain with z = 2 does not show any magnetic order even at zero temperature 6 , whereas long range order is possible at T = 0 in the 2D case 7 as, e.g., in the prominent S = 1/2 Heisenberg square lattice model with z = 4. The honeycomb lattice has the minimum possible coordination number of any regular 2D lattice z = 3. Thus quantum fluctuations there are weaker than in the 1D case, but stronger than in the 2D square lattice. Hence, the AFM order for the honeycomb lattice is fragile 8,9 .Experimentally, low-D spin systems described by the Heisenberg Hamiltonian H = 2J afm S i S j are often realized in structurally three dimensional organic-or transition metal oxide (TMO) compounds where strong AFM exchange interaction J afm between unpaired localized spins occurs along only one or two spacial directions. Owing to residual small 3D exchange couplings such materials usually exhibit a long range Néel order at a finite temperature T N , though, unlike in the 3D magnets, the ordering occurs at much smaller temperaturesRecently, a complex TMO compound, InCu 2/3 V 1/3 O 3 , was suggested as a possible candidate for the realization of the S = 1/2 honeycomb lattice 10 . In its layered hexagonal structure the Cu 2+ (3d 9...