<?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/18074'>
    <docid>18074</docid>
    <rev_number>2</rev_number>
    <files>
      <file id='https://researchdata.bath.ac.uk/id/file/68809'>
        <fileid>68809</fileid>
        <datasetid>document</datasetid>
        <objectid>18074</objectid>
        <filename>FigS6a_fNBO_vs_density_no-initial_NBO_Al4_v2.agr</filename>
        <mime_type>text/plain</mime_type>
        <hash>1c321b5e70085a5cd1edde595cfbeeaf</hash>
        <hash_type>MD5</hash_type>
        <filesize>23243</filesize>
        <mtime>2024-06-15 15:22:53</mtime>
        <url>https://researchdata.bath.ac.uk/1387/67/FigS6a_fNBO_vs_density_no-initial_NBO_Al4_v2.agr</url>
      </file>
    </files>
    <eprintid>1387</eprintid>
    <pos>67</pos>
    <placement>67</placement>
    <mime_type>text/plain</mime_type>
    <format>other</format>
    <formatdesc>Figure S6(a) shows the dependence of the fraction of non-bridging oxygen atoms f_{NBO} on the reduced density rho^prime for the tectosilicate glasses with f_{NBO} ~0 at rho^prime = 1. The fraction of NBO atoms was calculated by assuming that f_{Si(IV)} = 1 and only the Si(IV) and Al(IV) species contribute towards the network.</formatdesc>
    <language>en</language>
    <security>public</security>
    <license>cc_by</license>
    <main>FigS6a_fNBO_vs_density_no-initial_NBO_Al4_v2.agr</main>
    <content>data</content>
  </document>
</documents>
