The current experimental efforts in accessing the spin solid state in artificial honeycomb lattice is mainly based on the employment of the electron‐beam lithography method for sample fabrication, which generally leads to small sample sizes with large elemental parameters. Such large element size honeycomb lattice typically manifests an inter‐elemental interaction energies of ≈104 K.1, 8, 9, 10 More recently, a new design of artificial honeycomb lattice, consisting of very thin (few angstroms) and well‐separated permalloy elements of large size (≈500 nm in length and 20–50 nm in width) that reduces the interelemental energy significantly, was proposed to access the spin solid state in the disconnected geometry.11, 12 In the disconnected honeycomb lattice, the underlying physics is dictated by the Block transition mechanism. On the other hand, the physical connection between the lattice elements in connected honeycomb lattice facilitates the propagation of domain wall from one vertex to another, which is necessary for inducing the spin flip and, hence, the continuous progression of a new magnetic phase as temperature is reduced.8, 13, 14 Here, we take a different approach and create large throughput new artificial honeycomb lattice of connected ultrasmall elements. The ultrasmall size of the connecting elements automatically reduces the interelemental magnetostatic energy between 12 and 15 K. Therefore, it is quite suitable for the investigation of temperature‐dependent evolution of magnetic phases using reciprocal space probes, such as neutron scattering method.