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
MARC21 XML Export
<?xml version='1.0' encoding='UTF-8'?>
<record xmlns="http://www.loc.gov/MARC21/slim">
<leader>00000nmm##2200000uu#4500</leader>
<datafield tag="100" ind1=" " ind2=" ">
<subfield code="a">Körber, Lukas</subfield>
<subfield code="u">TU Dresden</subfield>
<subfield code="0">(orcid)0000-0001-8332-9669</subfield>
</datafield>
<controlfield tag="001">1278</controlfield>
<datafield tag="909" ind1="C" ind2="O">
<subfield code="o">oai:rodare.hzdr.de:1278</subfield>
<subfield code="p">openaire_data</subfield>
<subfield code="p">user-rodare</subfield>
</datafield>
<datafield tag="520" ind1=" " ind2=" ">
<subfield code="a"><p>This dataset contains the experimental and numerical raw data for our publication &quot;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;Symmetry- and curvature effects on spin waves in vortex-state hexagonal nanotubes&quot;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt; published in Physical Review B. The experimental data is described in detail in the PDF &quot;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;MAXYMUS_Tube210nm_antje500nm_2017_10_14&quot;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;.&nbsp;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;nbsp&amp;&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;lt&gt;&amp;&amp;&gt;lt&gt;nbsp&amp;&gt;lt&gt;</p>
<p>&nbsp;</p>
<p>The dynamic matrix data contains eparam.yaml and sparam.yaml files containing the simulation and sample parameters used for micromagnetic modeling.</p></subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">spin wave</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">dispersion</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">curvature</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">micromagnetic modeling</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">hexagonal</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">symmetry</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">STXM</subfield>
</datafield>
<datafield tag="024" ind1=" " ind2=" ">
<subfield code="a">10.14278/rodare.1278</subfield>
<subfield code="2">doi</subfield>
</datafield>
<datafield tag="542" ind1=" " ind2=" ">
<subfield code="l">open</subfield>
</datafield>
<datafield tag="650" ind1="1" ind2="7">
<subfield code="a">cc-by</subfield>
<subfield code="2">opendefinition.org</subfield>
</datafield>
<datafield tag="540" ind1=" " ind2=" ">
<subfield code="u">https://creativecommons.org/licenses/by/4.0/legalcode</subfield>
<subfield code="a">Creative Commons Attribution 4.0 International</subfield>
</datafield>
<datafield tag="856" ind1="4" ind2=" ">
<subfield code="s">102667930</subfield>
<subfield code="u">https://rodare.hzdr.de/record/1278/files/Archive.zip</subfield>
<subfield code="z">md5:d3f3e0ac551cd482991acb75e0acc416</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Zimmermann, Michael</subfield>
<subfield code="u">Uni Regensburg</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Wintz, Sebastian</subfield>
<subfield code="u">PSI, MPI für Intelligente Systeme Stuttgart</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Finizio, Simone</subfield>
<subfield code="u">PSI</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Kronseder, Matthias</subfield>
<subfield code="u">Uni Regensburg</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Bougeard, Dominique</subfield>
<subfield code="u">Uni Regensburg</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Dirnberger, Florian</subfield>
<subfield code="u">Uni Regensburg</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Weigand, Markus</subfield>
<subfield code="u">MPI für Intelligente Systeme Stuttgart, Helmholtz-Zentrum Berlin</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Raabe, Jörg</subfield>
<subfield code="u">PSI</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Otálora, Jorge A.</subfield>
<subfield code="u">Universidad Catálica del Norte Chile</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Schultheiß, Helmut</subfield>
<subfield code="u">TU Dresden</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Josten, Elisabeth</subfield>
<subfield code="u">FZ Jülich</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Lindner, Jürgen</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Kézsmárki, István</subfield>
<subfield code="u">Uni Augsburg</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Back, Christian H.</subfield>
<subfield code="u">Uni Regensburg, TU München</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Kakay, Attila</subfield>
<subfield code="0">(orcid)0000-0002-3195-219X</subfield>
</datafield>
<datafield tag="773" ind1=" " ind2=" ">
<subfield code="a">10.1103/PhysRevB.104.184429</subfield>
<subfield code="i">isReferencedBy</subfield>
<subfield code="n">doi</subfield>
</datafield>
<datafield tag="773" ind1=" " ind2=" ">
<subfield code="a">https://www.hzdr.de/publications/Publ-33367</subfield>
<subfield code="i">isReferencedBy</subfield>
<subfield code="n">url</subfield>
</datafield>
<datafield tag="773" ind1=" " ind2=" ">
<subfield code="a">https://www.hzdr.de/publications/Publ-33475</subfield>
<subfield code="i">isIdenticalTo</subfield>
<subfield code="n">url</subfield>
</datafield>
<datafield tag="773" ind1=" " ind2=" ">
<subfield code="a">10.14278/rodare.1277</subfield>
<subfield code="i">isVersionOf</subfield>
<subfield code="n">doi</subfield>
</datafield>
<datafield tag="980" ind1=" " ind2=" ">
<subfield code="a">dataset</subfield>
</datafield>
<controlfield tag="005">20230127125449.0</controlfield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="a">Data publication: Symmetry and curvature effects on spin waves in vortex-state hexagonal nanotubes</subfield>
</datafield>
<datafield tag="260" ind1=" " ind2=" ">
<subfield code="c">2021-11-26</subfield>
</datafield>
<datafield tag="980" ind1=" " ind2=" ">
<subfield code="a">user-rodare</subfield>
</datafield>
</record>
416
158
views
downloads
| All versions | This version | |
|---|---|---|
| Views | 416 | 416 |
| Downloads | 158 | 158 |
| Data volume | 16.2 GB | 16.2 GB |
| Unique views | 177 | 177 |
| Unique downloads | 22 | 22 |
- Publication date:
- November 26, 2021
- DOI:
-
- 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 - Communities:
- License (for files):
- Creative Commons Attribution 4.0 International