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Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
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Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
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Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
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Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem
Journal Article

Switchable geometric frustration in an artificial-spin-ice–superconductor heterosystem

2018
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Overview
Geometric frustration emerges when local interaction energies in an ordered lattice structure cannot be simultaneously minimized, resulting in a large number of degenerate states. The numerous degenerate configurations may lead to practical applications in microelectronics1, such as data storage, memory and logic2. However, it is difficult to achieve very high degeneracy, especially in a two-dimensional system3,4. Here, we showcase in situ controllable geometric frustration with high degeneracy in a two-dimensional flux-quantum system. We create this in a superconducting thin film placed underneath a reconfigurable artificial-spin-ice structure5. The tunable magnetic charges in the artificial-spin-ice strongly interact with the flux quanta in the superconductor, enabling switching between frustrated and crystallized flux quanta states. The different states have measurable effects on the superconducting critical current profile, which can be reconfigured by precise selection of the spin-ice magnetic state through the application of an external magnetic field. We demonstrate the applicability of these effects by realizing a reprogrammable flux quanta diode. The tailoring of the energy landscape of interacting ‘particles’ using artificial-spin-ices provides a new paradigm for the design of geometric frustration, which could illuminate a path to control new functionalities in other material systems, such as magnetic skyrmions6, electrons and holes in two-dimensional materials7,8, and topological insulators9, as well as colloids in soft materials10–13.