Architectural materials at mesoscale open new opportunitiesfor the design of materials with unique combinations of properties. [1][2][3] One of the subclasses of this kind of material is lattice (meta)materials. Classical lattice materials have a mesh-like structure generated by translation in space of an elementary cell that comprises several, most commonly identical, elements, such as thin bars or rods. [4,5] It was found that materials with this type of inner architecture while having a low density, exhibit high values of stiffness, strength, and fracture toughness. [4][5][6] Great expectations in this field are connected with nanoscale lattices. [7,8] Two principal directions can be followed to get to more versatile behavior. First, lattice-based metamaterials can, of course, be built from more complex unit cells. Buckling elements in the unit cell can effectively give a plastic response, [9] chiral elements can show macroscopically chiral response, [10] and gear-based lattice structures can change connectivity and allow extreme adaptivity of elastic properties even in the built structure. [11] The second direction is to build lattice materials with a structure different from the classical one, which possesses new properties. [12] For example, it was shown that irregular mesh