<?xml version='1.0' encoding='utf-8'?>
<documents xmlns='http://eprints.org/ep2/data/2.0'>
  <document id='https://researchdata.bath.ac.uk/id/document/15461'>
    <docid>15461</docid>
    <rev_number>2</rev_number>
    <files>
      <file id='https://researchdata.bath.ac.uk/id/file/50027'>
        <fileid>50027</fileid>
        <datasetid>document</datasetid>
        <objectid>15461</objectid>
        <filename>thesis_fig_5_8_archive.zip</filename>
        <mime_type>application/zip</mime_type>
        <hash>8db0e926d4527d28507c6b9d89e4d9c5</hash>
        <hash_type>MD5</hash_type>
        <filesize>89593279</filesize>
        <mtime>2021-11-09 15:33:46</mtime>
        <url>https://researchdata.bath.ac.uk/1089/4/thesis_fig_5_8_archive.zip</url>
      </file>
    </files>
    <eprintid>1089</eprintid>
    <pos>4</pos>
    <placement>4</placement>
    <mime_type>application/zip</mime_type>
    <format>other</format>
    <formatdesc>Folder containing data for simulations and predictions shown in Fig.5-8 of the thesis. This figure shows a comparison between predictions and simulations of the Raman-induced frequency shift (and associated acceleration) of a soliton. In this figure dispersion is set to be normal and much greater in the the second harmonic compared to the fundamental frequency (s_2&gt;r_2 as defined in the thesis).</formatdesc>
    <language>en</language>
    <security>public</security>
    <license>cc_by</license>
    <main>thesis_fig_5_8_archive.zip</main>
    <content>data</content>
  </document>
</documents>
