Dataset Open Access

Data publication: Symmetry and curvature effects on spin waves in vortex-state hexagonal nanotubes

Körber, Lukas; Zimmermann, Michael; Wintz, Sebastian; Finizio, Simone; Kronseder, Matthias; Bougeard, Dominique; Dirnberger, Florian; Weigand, Markus; Raabe, Jörg; Otálora, Jorge A.; Schultheiß, Helmut; Josten, Elisabeth; Lindner, Jürgen; Kézsmárki, István; Back, Christian H.; Kakay, Attila

This dataset contains the experimental and numerical raw data for our publication "&&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>Symmetry- and curvature effects on spin waves in vortex-state hexagonal nanotubes"&&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt> published in Physical Review B. The experimental data is described in detail in the PDF "&&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>MAXYMUS_Tube210nm_antje500nm_2017_10_14"&&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>. &&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>lt>&&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>nbsp&>&&>lt>nbsp&>lt>lt>&&>lt>nbsp&>lt>

 

The dynamic matrix data contains eparam.yaml and sparam.yaml files containing the simulation and sample parameters used for micromagnetic modeling.

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Publication date:
November 26, 2021
DOI:
10.14278/rodare.1278

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Keyword(s):
spin wave dispersion curvature micromagnetic modeling hexagonal symmetry STXM
Related identifiers:
Identical to:
https://www.hzdr.de/publications/Publ-33475
Referenced by:
10.1103/PhysRevB.104.184429, https://www.hzdr.de/publications/Publ-33367
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License (for files):
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