2020
DOI: 10.1103/physrevb.102.180405
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Thermally superactive artificial kagome spin ice structures obtained with the interfacial Dzyaloshinskii-Moriya interaction

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Cited by 21 publications
(10 citation statements)
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“…The latter is particularly important for solving issues related to the ordering and thermal excitations of coupled mesospins. 13,[32][33][34] This knowledge may even find its application in logic and computation, 35 such as design of neuromorphic-like architectures based on ASIs and their magnonic properties. 36 See the supplementary material for the details concerning the comparison of magnon mode frequencies to analytic expressions.…”
mentioning
confidence: 99%
“…The latter is particularly important for solving issues related to the ordering and thermal excitations of coupled mesospins. 13,[32][33][34] This knowledge may even find its application in logic and computation, 35 such as design of neuromorphic-like architectures based on ASIs and their magnonic properties. 36 See the supplementary material for the details concerning the comparison of magnon mode frequencies to analytic expressions.…”
mentioning
confidence: 99%
“…For the frustrated system with an Ising model, from geometry or lattice, even in the ground state, there can be multiple degenerated. In the ground state, there are pair interaction energies E i j that are unfavorable (i.e., similar to other frustrated systems like the kagome system [65]). This means that there are more possible states with a ground-state energy, and, more important, that there is a special lowest energy value,…”
Section: Model and Computational Methodsmentioning
confidence: 88%
“…9(b)]. It is obvious that the experimental system attempts to access a long-range ordered ground state, but as shown in previous studies on various artificial frustrated spin systems, fabrication-related intrinsic disorder, and the blocking temperature of the nanomagnets can significantly slow down and hinder relaxation towards a long-range ordered ground state [64,65,68]. The free energy minimum must correspond to stable thermodynamic equilibrium and the realization of the most probable state.…”
Section: Discussionmentioning
confidence: 99%
“…It exhibits various competing interactions, which can be directly controlled by the lattice parameter b. Tuning of the strengths of the interactions allows it to transition from a long-range ordered ground state dominated by clockwiseand anticlockwise vortices, through a highly disordered state, when competing interactions are equalized, to a phase manifested by an increasing ice-rule obedience and a preference for ferromagnetic-type moment alignments. The variety of ordering preferences as interactions J 1 and J 2 are varied and equalized pose interesting questions, regarding its ground state and potential phase transitions at lower or higher temperatures, which can be either addressed via simulations [41,53,54] or experimentally, if structures with lowered block-ing temperatures can be generated [55]. Newly emerging coherent x-ray scattering techniques [56] appear to be the best method for shedding light on these open questions.…”
Section: Discussionmentioning
confidence: 99%