{"data":{"id":"10.5442/nd000001","type":"dois","attributes":{"doi":"10.5442/nd000001","prefix":"10.5442","suffix":"nd000001","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Hoffmann, J.-U.","nameType":"Personal","givenName":"J.-U.","familyName":"Hoffmann","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-3651-958X","nameIdentifierScheme":"ORCID"}]},{"name":"Siemensmeyer, K.","nameType":"Personal","givenName":"K.","familyName":"Siemensmeyer","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-7271-7989","nameIdentifierScheme":"ORCID"}]},{"name":"Isakov, S.","nameType":"Personal","givenName":"S.","familyName":"Isakov","affiliation":["Theoretische Physik, ETH Zürich, 8093 Zürich, Switzerland","Google Inc., Brandschenkestrasse 110, 8002 Zürich, Switzerland"],"nameIdentifiers":[]},{"name":"Morris, D. J. P.","nameType":"Personal","givenName":"D. J. P.","familyName":"Morris","affiliation":["Xavier University, Department of Physics, 3800 Victory Parkway, Cincinnati, OH 45207, USA"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-4785-7541","nameIdentifierScheme":"ORCID"}]},{"name":"Klemke, B.","nameType":"Personal","givenName":"B.","familyName":"Klemke","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-4560-6025","nameIdentifierScheme":"ORCID"}]},{"name":"Glavatskyi, I.","nameType":"Personal","givenName":"I.","familyName":"Glavatskyi","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany","Scienion AG, Volmerstr. 7b, 12489 Berlin, Germany"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-5853-3542","nameIdentifierScheme":"ORCID"}]},{"name":"Seiffert, K.","nameType":"Personal","givenName":"K.","familyName":"Seiffert","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany","Technische Universität Berlin, Pascalstr. 8-9, 10587 Berlin, Germany"],"nameIdentifiers":[]},{"name":"Tennant, D. A.","nameType":"Personal","givenName":"D. A.","familyName":"Tennant","affiliation":["Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany","Oak Ridge National Laboratory, PO Box 2008 MS-6477, Oak Ridge, TN 37831, USA"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-9575-3368","nameIdentifierScheme":"ORCID"}]},{"name":"Sondhi, S.","nameType":"Personal","givenName":"S.","familyName":"Sondhi","affiliation":["Dept. of Physics, Princeton University, Washington Road, Princeton, NJ 08544, USA"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0001-9154-6102","nameIdentifierScheme":"ORCID"}]},{"name":"Moessner, R.","nameType":"Personal","givenName":"R.","familyName":"Moessner","affiliation":["Max-Planck-Institut für Physik komplexer Systeme, Nöthnitzer Straße 38, 01187 Dresden, Germany"],"nameIdentifiers":[]}],"titles":[{"title":"Neutron study of the topological flux model of hydrogen ions in water ice"}],"publisher":"HZB Data Service","container":{},"publicationYear":2018,"subjects":[{"subject":"neutron diffraction","valueUri":"http://purl.org/pan-science/PaNET/PaNET01217","schemeUri":"http://purl.org/pan-science/PaNET/","subjectScheme":"The Photon and Neutron Experimental Techniques Ontology"}],"contributors":[],"dates":[{"date":"2018","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsCitedBy","relatedIdentifier":"10.1103/physrevb.99.174111","relatedIdentifierType":"DOI"},{"relationType":"References","relatedIdentifier":"10.17815/jlsrf-4-110","relatedIdentifierType":"DOI"},{"relationType":"IsCollectedBy","relatedIdentifier":"10.5442/ni000001","relatedIdentifierType":"DOI"}],"relatedItems":[{"titles":[{"title":"Neutron studies of gauge field and charge in Ih heavy-water ice"}],"creators":[],"contributors":[],"relationType":"IsCitedBy","relatedItemType":"JournalArticle","relatedItemIdentifier":{"relatedItemIdentifier":"10.1103/physrevb.99.174111","relatedItemIdentifierType":"DOI"}},{"titles":[{"title":"E2: The Flat-Cone Diffractometer at BER II"}],"creators":[],"contributors":[],"relationType":"References","relatedItemType":"JournalArticle","relatedItemIdentifier":{"relatedItemIdentifier":"10.17815/jlsrf-4-110","relatedItemIdentifierType":"DOI"}},{"titles":[{"title":"E2 - Flat-Cone Diffractometer"}],"creators":[],"contributors":[],"relationType":"IsCollectedBy","relatedItemType":"Instrument","relatedItemIdentifier":{"relatedItemIdentifier":"10.5442/ni000001","relatedItemIdentifierType":"DOI"}}],"sizes":["1.23 GiB"],"formats":["application/x-hdf5"],"version":null,"rightsList":[{"rights":"Creative Commons Zero v1.0 Universal","rightsUri":"https://creativecommons.org/publicdomain/zero/1.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc0-1.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"The familiarity of water ice means we often overlook its non-trivial character illustrated, for example, by the many snowflake morphologies resulting from disordered combinations of covalent and hydrogen bonds between hydrogen and oxygen atoms in water ice’s most common phase (Ih) that keep the H_2 O molecular character. Using neutron diffraction on the flat-cone diffractometer E2 at BER-II, Helmholtz-Zentrum Berlin, we probe the atomic scale configuration in the Ih phase of water ice to test theories that describe this “disordered” state as exhibiting a form of topological order characterized by an emergent gauge field. We find excellent agreement between low-temperature experiment and analytical theory, which even allows us to estimate the density of defects charged under this emergent gauge field. The development of quantitative models of water ice paves the way for further studies to develop a comprehensive atomic-scale understanding of this most commonplace of solids.\nThe merged untransformed datasets from the flat-cone diffractometer E2 at the neutron source BER II is given in the Nexus/HDF5 file format. The calculated reciprocal space and the simulation are stored as HDF5 files.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"<?xml version="1.0" encoding="UTF-8"?>
<resource xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns="http://datacite.org/schema/kernel-4" xsi:schemaLocation="http://datacite.org/schema/kernel-4 https://schema.datacite.org/meta/kernel-4.5/metadata.xsd">
  <identifier identifierType="DOI">10.5442/ND000001</identifier>
  <creators>
    <creator>
      <creatorName nameType="Personal">Hoffmann, J.-U.</creatorName>
      <givenName>J.-U.</givenName>
      <familyName>Hoffmann</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0002-3651-958X</nameIdentifier>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Siemensmeyer, K.</creatorName>
      <givenName>K.</givenName>
      <familyName>Siemensmeyer</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0002-7271-7989</nameIdentifier>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Isakov, S.</creatorName>
      <givenName>S.</givenName>
      <familyName>Isakov</familyName>
      <affiliation affiliationIdentifier="05a28rw58" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Theoretische Physik, ETH Zürich, 8093 Zürich, Switzerland</affiliation>
      <affiliation affiliationIdentifier="014f9c269" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Google Inc., Brandschenkestrasse 110, 8002 Zürich, Switzerland</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Morris, D. J. P.</creatorName>
      <givenName>D. J. P.</givenName>
      <familyName>Morris</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0002-4785-7541</nameIdentifier>
      <affiliation affiliationIdentifier="00f266q65" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Xavier University, Department of Physics, 3800 Victory Parkway, Cincinnati, OH 45207, USA</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Klemke, B.</creatorName>
      <givenName>B.</givenName>
      <familyName>Klemke</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0003-4560-6025</nameIdentifier>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Glavatskyi, I.</creatorName>
      <givenName>I.</givenName>
      <familyName>Glavatskyi</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0002-5853-3542</nameIdentifier>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
      <affiliation affiliationIdentifier="04h03k610" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Scienion AG, Volmerstr. 7b, 12489 Berlin, Germany</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Seiffert, K.</creatorName>
      <givenName>K.</givenName>
      <familyName>Seiffert</familyName>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
      <affiliation affiliationIdentifier="03v4gjf40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Technische Universität Berlin, Pascalstr. 8-9, 10587 Berlin, Germany</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Tennant, D. A.</creatorName>
      <givenName>D. A.</givenName>
      <familyName>Tennant</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0002-9575-3368</nameIdentifier>
      <affiliation affiliationIdentifier="02aj13c28" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, 14109 Berlin, Germany</affiliation>
      <affiliation affiliationIdentifier="01qz5mb56" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Oak Ridge National Laboratory, PO Box 2008 MS-6477, Oak Ridge, TN 37831, USA</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Sondhi, S.</creatorName>
      <givenName>S.</givenName>
      <familyName>Sondhi</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="https://orcid.org/">0000-0001-9154-6102</nameIdentifier>
      <affiliation affiliationIdentifier="00hx57361" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Dept. of Physics, Princeton University, Washington Road, Princeton, NJ 08544, USA</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Moessner, R.</creatorName>
      <givenName>R.</givenName>
      <familyName>Moessner</familyName>
      <affiliation affiliationIdentifier="01bf9rw71" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org/">Max-Planck-Institut für Physik komplexer Systeme, Nöthnitzer Straße 38, 01187 Dresden, Germany</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Neutron study of the topological flux model of hydrogen ions in water ice</title>
  </titles>
  <publisher>HZB Data Service</publisher>
  <publicationYear>2018</publicationYear>
  <subjects>
    <subject schemeURI="http://purl.org/pan-science/PaNET/" subjectScheme="The Photon and Neutron Experimental Techniques Ontology" valueURI="http://purl.org/pan-science/PaNET/PaNET01217">neutron diffraction</subject>
  </subjects>
  <resourceType resourceTypeGeneral="Dataset">Dataset</resourceType>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsCitedBy">10.1103/physrevb.99.174111</relatedIdentifier>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="References">10.17815/jlsrf-4-110</relatedIdentifier>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsCollectedBy">10.5442/NI000001</relatedIdentifier>
  </relatedIdentifiers>
  <sizes>
    <size>1.23 GiB</size>
  </sizes>
  <formats>
    <format>application/x-hdf5</format>
  </formats>
  <rightsList>
    <rights rightsURI="https://creativecommons.org/publicdomain/zero/1.0/" rightsIdentifier="CC0-1.0" rightsIdentifierScheme="SPDX">Creative Commons Zero v1.0 Universal</rights>
  </rightsList>
  <descriptions>
    <description descriptionType="Abstract">The familiarity of water ice means we often overlook its non-trivial character illustrated, for example, by the many snowflake morphologies resulting from disordered combinations of covalent and hydrogen bonds between hydrogen and oxygen atoms in water ice’s most common phase (Ih) that keep the H_2 O molecular character. Using neutron diffraction on the flat-cone diffractometer E2 at BER-II, Helmholtz-Zentrum Berlin, we probe the atomic scale configuration in the Ih phase of water ice to test theories that describe this “disordered” state as exhibiting a form of topological order characterized by an emergent gauge field. We find excellent agreement between low-temperature experiment and analytical theory, which even allows us to estimate the density of defects charged under this emergent gauge field. The development of quantitative models of water ice paves the way for further studies to develop a comprehensive atomic-scale understanding of this most commonplace of solids.
The merged untransformed datasets from the flat-cone diffractometer E2 at the neutron source BER II is given in the Nexus/HDF5 file format. The calculated reciprocal space and the simulation are stored as HDF5 files.</description>
  </descriptions>
  <relatedItems>
    <relatedItem relatedItemType="JournalArticle" relationType="IsCitedBy">
      <relatedItemIdentifier relatedItemIdentifierType="DOI">10.1103/physrevb.99.174111</relatedItemIdentifier>
      <titles>
        <title>Neutron studies of gauge field and charge in Ih heavy-water ice</title>
      </titles>
    </relatedItem>
    <relatedItem relatedItemType="JournalArticle" relationType="References">
      <relatedItemIdentifier relatedItemIdentifierType="DOI">10.17815/jlsrf-4-110</relatedItemIdentifier>
      <titles>
        <title>E2: The Flat-Cone Diffractometer at BER II</title>
      </titles>
    </relatedItem>
    <relatedItem relatedItemType="Instrument" relationType="IsCollectedBy">
      <relatedItemIdentifier relatedItemIdentifierType="DOI">10.5442/NI000001</relatedItemIdentifier>
      <titles>
        <title>E2 - Flat-Cone Diffractometer</title>
      </titles>
    </relatedItem>
  </relatedItems>
</resource>","url":"https://data.helmholtz-berlin.de/pub/ND000001","contentUrl":null,"metadataVersion":9,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":2,"citationCount":1,"citationsOverTime":[{"year":"2019","total":1}],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2018-03-06T14:07:24.000Z","registered":"2018-03-06T14:07:24.000Z","published":"2018","updated":"2024-04-19T15:25:33.000Z"},"relationships":{"client":{"data":{"id":"tib.hzb","type":"clients"}},"provider":{"data":{"id":"dxdt","type":"providers"}},"media":{"data":{"id":"10.5442/nd000001","type":"media"}},"references":{"data":[{"id":"10.17815/jlsrf-4-110","type":"dois"},{"id":"10.1103/physrevb.99.174111","type":"dois"}]},"citations":{"data":[{"id":"10.1103/physrevb.99.174111","type":"dois"}]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}