Artificial spin ice is a frustrated magnetic two-dimensional nano-material, recently employed to study variety of tailor-designed unusual collective behaviours. Recently proposed extensions to three dimensions are based on self-assembly techniques and allow little control over geometry and disorder. We present a viable design for the realization of a three-dimensional artificial spin ice with the same level of precision and control allowed by lithographic nano-fabrication of the popular two-dimensional case. Our geometry is based on layering already available two-dimensional artificial spin ice and leads to an arrangement of ice-rule-frustrated units which is topologically equivalent to that of the tetrahedra in a pyrochlore lattice. Consequently, we show, it exhibits a genuine ice phase and its excitations are, as in natural spin ice materials, magnetic monopoles interacting via Coulomb law.
PACS numbers:Spin ice materials, such as rare-earth pyrochlores and artificial spin ice, are magnetic systems in which frustrated interactions lead to complex (partial) orderings and unusual collective behaviours [1][2][3]. Magnetic ions in pyrochlore spin ice form a network of corner-sharing tetrahedra whose classical magnetic macro-spins minimize the local interaction energy by obeying the twoin-two-out ice rule proposed by Pauling for the proton orderings in water ice [4]: hence the name, spin ice. It has recently been demonstrated that elementary excitations over the disordered ice manifold of spin ice materials are emergent magnetic monopoles that fractionalize from local dipole excitations [5,6].The artificial counterparts of these natural materials, artificial spin ices [3,7], are nanostructured twodimensional (2D) arrays of single-domain ferromagnetic bars that behave like giant Ising spins. Collective behaviour of the nanomagnets can be controlled through appropriate choices of material, geometry and array topology. Because of their nano-scale interaction energies (∼ 10 3 − 10 5 K depending on the size of the nanomagnet and mutual spacing) they reveal, at accessible temperatures, emergent features which in natural materials are seen only at very low temperature. Following the pioneering work of Wang et al. on the two-dimensional square-ice array [7,8], artificial spin ices have been proposed and studied in diverse types of physical systems [9][10][11][12] and geometries such as honeycomb (kagome ice) [13][14][15][16][17][18][19][20], brickwork [21], triangular [22][23][24], and pentagonal lattices [25]. A systematic approach for designing 2D arrays with emergent ice-type frustration has also been proposed [26,27], and recently realized experimentally [29].Most of the experimental efforts in such artificial frustrated magnets has understandably focused on twodimensional systems: even with mature nanolithography, it remains a great challenge to integrate a full three-dimensional (3D) structure with oblique angles between nanobars such as the pyrochlore lattice. Recently an interesting realization of a 3D artificial s...