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1 scopic insight into this novel geometrically frustrated system.
2 in free energy landscapes characteristic of frustrated systems.
3 hinting at the role of kinetic magnetism in frustrated systems.
11 cenario might be expected to occur widely in frustrated systems containing first-order phase transiti
12 y peaked at intermediate phi, whereas highly frustrated systems display a bimodal distribution peaked
20 , we provide a first look into an artificial frustrated system, the dipolar trident lattice, where th
22 mpound, [Formula: see text], a geometrically frustrated system with effective spin-1/2 local moments
23 perfect match to the expected behavior for a frustrated system with the lowest energy pair of S=1/2 s
24 These results highlight how a geometrically frustrated system, with thermodynamics strictly adhering