{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,18]],"date-time":"2026-09-18T19:02:45Z","timestamp":1789758165890,"version":"4.0.1"},"reference-count":23,"publisher":"AIP Publishing","issue":"5","license":[{"start":{"date-parts":[[2017,12,22]],"date-time":"2017-12-22T00:00:00Z","timestamp":1513900800000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"},{"start":{"date-parts":[[2017,12,22]],"date-time":"2017-12-22T00:00:00Z","timestamp":1513900800000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"short-container-title":[],"published-print":{"date-parts":[[2018,5,1]]},"abstract":"<jats:p>We study a crystal of skyrmions generated on a square lattice using a ferromagnetic exchange interaction and a Dzyaloshinskii-Moriya interaction between nearest-neighbors under an external magnetic field. The skyrmion crystal has a hexagonal structure which is shown to be stable up to a temperature Tc where a transition to the paramagnetic phase occur. We will show that the dynamics of the skyrmions at T &amp;lt; Tc follows a stretched exponential law.<\/jats:p>","DOI":"10.1063\/1.5006269","type":"journal-article","created":{"date-parts":[[2017,12,22]],"date-time":"2017-12-22T15:11:25Z","timestamp":1513955485000},"update-policy":"https:\/\/doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":8,"title":["Skyrmion crystals: Dynamics and phase transition"],"prefix":"10.1063","volume":"8","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-1852-3435","authenticated-orcid":false,"given":"H. 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