{"data":{"id":"10.5061/dryad.4tmpg4frb","type":"dois","attributes":{"doi":"10.5061/dryad.4tmpg4frb","prefix":"10.5061","suffix":"dryad.4tmpg4frb","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Roy, Sujoy","nameType":"Personal","givenName":"Sujoy","familyName":"Roy","affiliation":["Lawrence Berkeley National Laboratory"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-5695-7894","nameIdentifierScheme":"ORCID"}]},{"name":"Atkar, Soham","nameType":"Personal","givenName":"Soham","familyName":"Atkar","affiliation":["Indian Institute of Technology Guwahati"],"nameIdentifiers":[]},{"name":"Datta, Trinanjan","nameType":"Personal","givenName":"Trinanjan","familyName":"Datta","affiliation":["Augusta University"],"nameIdentifiers":[]},{"name":"Tumbleson, Z.","nameType":"Personal","givenName":"Z.","familyName":"Tumbleson","affiliation":["University of California, Santa Cruz"],"nameIdentifiers":[]},{"name":"Morley, Sophie","nameType":"Personal","givenName":"Sophie","familyName":"Morley","affiliation":["Lawrence Berkeley National Laboratory"],"nameIdentifiers":[]},{"name":"Burdet, N.","nameType":"Personal","givenName":"N.","familyName":"Burdet","affiliation":["SLAC National Accelerator Laboratory"],"nameIdentifiers":[]},{"name":"Islegen-Wojdyla, Antoine","nameType":"Personal","givenName":"Antoine","familyName":"Islegen-Wojdyla","affiliation":["Lawrence Berkeley National Laboratory"],"nameIdentifiers":[]},{"name":"Goldberg, Ken","nameType":"Personal","givenName":"Ken","familyName":"Goldberg","affiliation":["Lawrence Berkeley National Laboratory"],"nameIdentifiers":[]},{"name":"Scholl, A.","nameType":"Personal","givenName":"A.","familyName":"Scholl","affiliation":["Lawrence Berkeley National Laboratory"],"nameIdentifiers":[]},{"name":"Montoya, S. A","nameType":"Personal","givenName":"S. A","familyName":"Montoya","affiliation":["University of California San Diego"],"nameIdentifiers":[]}],"titles":[{"title":"Data from: Magnetically modified double slit-based X-ray interferometry"}],"publisher":"Dryad","container":{},"publicationYear":2026,"subjects":[{"subject":"XMCD"},{"subject":"Diffraction","schemeUri":"https://github.com/PLOS/plos-thesaurus","subjectScheme":"PLOS Subject Area Thesaurus"},{"subject":"FOS: Materials engineering","schemeUri":"https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf","subjectScheme":"fos"},{"subject":"FOS: Materials engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Nano-technology","schemeUri":"https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf","subjectScheme":"fos"},{"subject":"FOS: Physical sciences","schemeUri":"https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf","subjectScheme":"fos"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Optics","schemeUri":"https://github.com/PLOS/plos-thesaurus","subjectScheme":"PLOS Subject Area Thesaurus"}],"contributors":[{"name":"Advanced Light Source","affiliation":[],"contributorType":"Sponsor","nameIdentifiers":[]}],"dates":[{"date":"2026-02-21T00:32:45Z","dateType":"Created"},{"date":"2026-02-27T17:13:35Z","dateType":"Submitted"},{"date":"2026-03-25T00:00:00Z","dateType":"Issued"},{"date":"2026-03-25T00:00:00Z","dateType":"Available"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsCitedBy","relatedIdentifier":"10.1103/5njk-mhwg","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["66098 bytes"],"formats":[],"version":"6","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":"We performed x-ray based double slit diffraction with one of the slits\n covered with magnetic material. We then performed the experiment and\n collected double slit diffraction pattern as a function of external\n applied field. The dataset included here shows how the fringe moves as a\n function of applied field and how we can extract optical constant and\n ultimately relate to magnetization. ","descriptionType":"Abstract"},{"description":"# Data from: Magnetically modified double slit-based X-ray interferometry\n Dataset DOI:\n [10.5061/dryad.4tmpg4frb](https://doi.org/10.5061/dryad.4tmpg4frb) ##\n Description of the data and file structure Data was collected for\n X-ray-based double slit diffraction. The idea was to experimentally\n determine the fringe shift happening due to a change in the refractive\n index of a magnetic material under a magnetic field.  ### Files and\n variables #### Summary of Figure Data This dataset contains: 1. Fig 1b\n data: The data is a 1D linecut of the intensity interference-diffraction\n pattern. The normalized CCD data and normalized fit values are included\n and plotted against detector distance. 2. Fig 2 data: The data obtained\n from the registration algorithm to yield the fringe shifts for LCP and RCP\n light. The other data columns include derived values such as RCP - LCP.\n These values are scaled to show the fringe shift in terms of electron\n scattering factors. 3. Fig 3 data: Here, the data in the main panel is\n that of the beta value fits as a function of beam line energy obtained\n from the fitting algorithm. The inset is the absorption data obtained\n experimentally.  4. Fig 4 data: The inset shows the results of the\n registration algorithm values for the beam line energy scans. The main\n panel is the derivative of that data with respect to beam line energy to\n obtain the L3 absorption peak. ### File: data_description.rtf Description:\n A copy of the prior summary description in rich-text format ### File:\n fig1b_data.csv Description: A 1-dimensional line cut of the intensity\n pattern recorded by the CCD camera. The linecut was obtained by taking a\n small region along the x-axis (perpendicular to the pattern) and across\n the entire y-axis (along the pattern). The intensity data was normalized\n and is therefore scaled from 0 to 1. Using the fitting algorithm, we also\n plotted the fit values of the intensity to verify the obtained intensity\n function from Fraunhofer diffraction. #### Variables: Fit values: Obtained\n fit values of the intensity distribution along the y-axis.Data: The\n normalized data of the intensity distribution along the y-axis. Distance:\n The distance values across the y-axis on the CCD camera. ### File:\n fig2_data.csv Description: The registration algorithm tracked the physical\n movement of the fringes as the external magnetic field was varied in the\n out-of-plane direction with respect to the sample (z-axis). The data was\n recorded for LCP and RCP light. The dichroic signal (RCP - LCP) was also\n obtained. The fringe shift values were overlayed with curves that were\n smoothed using the Savitzky-Golay filter to emphasize the hysteresis loop\n behavior. The remainder of the data includes these fringe shift values\n scaled in terms of dispersive part of the refractive index. ####\n Variables: ΔY LCP: Lateral fringe shift of LCP light in µm ΔY LCP: Lateral\n fringe shift of LCP light smoothed using Savitzky-Golay filter in µm ΔY\n RCP: Lateral fringe shift of RCP light in µm ΔY RCP: Lateral fringe shift\n of RCP light smoothed using Savitzky-Golay filter in µm ΔY RCP-LCP: The\n dichroic signal fringe shift values in terms of the dispersive part of the\n refractive index in arbitrary units ΔY RCP-LCP: The dichroic signal fringe\n shift values smoothed using Savitzky-Golay filter in terms of the\n dispersive part of the refractive index in arbitrary units ΔY RCP-LCP: The\n dichroic signal fringe shift in terms of the electron scattering factors\n in arbitrary units. B_z: The applied external magnetic field applied in\n the out-of-plane direction with respect to the sample in Gauss. ### File:\n fig2_err.csv Description: The error values of the fringe shift values\n obtained from the registration algorithm for RCP and LCP light. ####\n Variables: LCP error: Error values for the fringe shifts with LCP light.\n RCP error: Error values for the fringe shifts with RCP light. ### File:\n fig3_data.csv Description: The beta values (absorptive part of the\n refractive index) are obtained from the fitting algorithm. These beta\n values are plotted as a function of the beam line energy to show the L2\n and L3 absorptive peaks. The inset shows complementary diode current data\n normalized to absorption. #### Variables: β(RCP): The imaginary part of\n the refractive index for RCP light β(LCP): The imaginary part of the\n refractive index for LCP light β(RCP-LCP): The dichroic signal of\n absorption in terms of imaginary part of the refractive index  Absorption\n (RCP): The diode current normalized to the absorption for RCP light\n Absorption (LCP): The diode current normalized to the absorption for LCP\n light Beamline energy (main panel): The beam line energy scale for the\n main panel 705 to 730 eV Beamline energy (inset panel): The beam line\n energy scale for the inset panel 695 to 735 eV ### File: fig4_data.csv\n Description: The inset displays the results of the registration algorithm\n applied to the beamline energy scans. The main panel presents the first\n derivative of this data with respect to the incident energy, effectively\n resolving the L3 absorption edge peak. #### Variables: ∂ΔY/∂E (LCP): The\n obtained fringe shift values are differentiated with respect to beamline\n energy to obtain the rate of fringe shift for LCP light in µm/eV ∂ΔY/∂E\n (RCP): The obtained fringe shift values are differentiated with respect to\n beamline energy to obtain the rate of fringe shift for RCP light in µm/eV\n ∂ΔY/∂E (RCP-LCP): The obtained dichroic fringe shift values are\n differentiated with respect to beamline energy to obtain the rate of\n fringe shift for the dichroic signal n µm/eV ΔY LCP: Lateral fringe shift\n of LCP light in µm ΔY RCP: Lateral fringe shift of RCP light in µm\n Beamline Energy: The beam line energy scale for both panels from 700 to\n 725 eV","descriptionType":"TechnicalInfo"}],"geoLocations":[],"fundingReferences":[{"schemeUri":"https://ror.org","funderName":"Advanced Research Projects Agency - Energy","funderIdentifier":"https://ror.org/03q1rgc19","funderIdentifierType":"ROR"}],"xml":"<?xml version="1.0" encoding="UTF-8"?>
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  <identifier identifierType="DOI">10.5061/DRYAD.4TMPG4FRB</identifier>
  <creators>
    <creator>
      <creatorName nameType="Personal">Roy, Sujoy</creatorName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0002-5695-7894</nameIdentifier>
      <affiliation affiliationIdentifier="https://ror.org/02jbv0t02" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Lawrence Berkeley National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Atkar, Soham</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/0022nd079" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Indian Institute of Technology Guwahati</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Datta, Trinanjan</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/012mef835" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Augusta University</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Tumbleson, Z.</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/03s65by71" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">University of California, Santa Cruz</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Morley, Sophie</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/02jbv0t02" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Lawrence Berkeley National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Burdet, N.</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/05gzmn429" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">SLAC National Accelerator Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Islegen-Wojdyla, Antoine</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/02jbv0t02" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Lawrence Berkeley National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Goldberg, Ken</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/02jbv0t02" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Lawrence Berkeley National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Scholl, A.</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/02jbv0t02" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Lawrence Berkeley National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName nameType="Personal">Montoya, S. A</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/0168r3w48" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">University of California San Diego</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Data from: Magnetically modified double slit-based X-ray interferometry</title>
  </titles>
  <publisher publisherIdentifier="https://ror.org/00x6h5n95" publisherIdentifierScheme="ROR" schemeURI="https://ror.org/">Dryad</publisher>
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  <publicationYear>2026</publicationYear>
  <subjects>
    <subject>XMCD</subject>
    <subject subjectScheme="PLOS Subject Area Thesaurus" schemeURI="https://github.com/PLOS/plos-thesaurus">Diffraction</subject>
    <subject subjectScheme="fos" schemeURI="https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf">FOS: Materials engineering</subject>
    <subject subjectScheme="fos" schemeURI="https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf">FOS: Nano-technology</subject>
    <subject subjectScheme="fos" schemeURI="https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf">FOS: Physical sciences</subject>
    <subject subjectScheme="PLOS Subject Area Thesaurus" schemeURI="https://github.com/PLOS/plos-thesaurus">Optics</subject>
  </subjects>
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      <funderName>Advanced Research Projects Agency - Energy</funderName>
      <funderIdentifier funderIdentifierType="ROR">https://ror.org/03q1rgc19</funderIdentifier>
      <awardTitle/>
    </fundingReference>
  </fundingReferences>
  <contributors>
    <contributor contributorType="Sponsor">
      <contributorName>Advanced Light Source</contributorName>
    </contributor>
  </contributors>
  <dates>
    <date dateType="Created">2026-02-21T00:32:45Z</date>
    <date dateType="Submitted">2026-02-27T17:13:35Z</date>
    <date dateType="Issued">2026-03-25T00:00:00Z</date>
    <date dateType="Available">2026-03-25T00:00:00Z</date>
  </dates>
  <language>en</language>
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  <descriptions>
    <description descriptionType="Abstract">
      We performed x-ray based double slit diffraction with one of the slits
      covered with magnetic material. We then performed the experiment and
      collected double slit diffraction pattern as a function of external
      applied field. The dataset included here shows how the fringe moves as a
      function of applied field and how we can extract optical constant and
      ultimately relate to magnetization.&amp;nbsp;
    </description>
    <description descriptionType="TechnicalInfo">
      # Data from: Magnetically modified double slit-based X-ray interferometry
      Dataset DOI:
      [10.5061/dryad.4tmpg4frb](https://doi.org/10.5061/dryad.4tmpg4frb) ##
      Description of the data and file structure Data was collected for
      X-ray-based double slit diffraction. The idea was to experimentally
      determine the fringe shift happening due to a change in the refractive
      index of a magnetic material under a magnetic field.  ### Files and
      variables #### Summary of Figure Data This dataset contains: 1. Fig 1b
      data: The data is a 1D linecut of the intensity interference-diffraction
      pattern. The normalized CCD data and normalized fit values are included
      and plotted against detector distance. 2. Fig 2 data: The data obtained
      from the registration algorithm to yield the fringe shifts for LCP and RCP
      light. The other data columns include derived values such as RCP - LCP.
      These values are scaled to show the fringe shift in terms of electron
      scattering factors. 3. Fig 3 data: Here, the data in the main panel is
      that of the beta value fits as a function of beam line energy obtained
      from the fitting algorithm. The inset is the absorption data obtained
      experimentally.  4. Fig 4 data: The inset shows the results of the
      registration algorithm values for the beam line energy scans. The main
      panel is the derivative of that data with respect to beam line energy to
      obtain the L3 absorption peak. ### File: data_description.rtf Description:
      A copy of the prior summary description in rich-text format ### File:
      fig1b_data.csv Description: A 1-dimensional line cut of the intensity
      pattern recorded by the CCD camera. The linecut was obtained by taking a
      small region along the x-axis (perpendicular to the pattern) and across
      the entire y-axis (along the pattern). The intensity data was normalized
      and is therefore scaled from 0 to 1. Using the fitting algorithm, we also
      plotted the fit values of the intensity to verify the obtained intensity
      function from Fraunhofer diffraction. #### Variables: Fit values: Obtained
      fit values of the intensity distribution along the y-axis.Data: The
      normalized data of the intensity distribution along the y-axis. Distance:
      The distance values across the y-axis on the CCD camera. ### File:
      fig2_data.csv Description: The registration algorithm tracked the physical
      movement of the fringes as the external magnetic field was varied in the
      out-of-plane direction with respect to the sample (z-axis). The data was
      recorded for LCP and RCP light. The dichroic signal (RCP - LCP) was also
      obtained. The fringe shift values were overlayed with curves that were
      smoothed using the Savitzky-Golay filter to emphasize the hysteresis loop
      behavior. The remainder of the data includes these fringe shift values
      scaled in terms of dispersive part of the refractive index. ####
      Variables: ΔY LCP: Lateral fringe shift of LCP light in µm ΔY LCP: Lateral
      fringe shift of LCP light smoothed using Savitzky-Golay filter in µm ΔY
      RCP: Lateral fringe shift of RCP light in µm ΔY RCP: Lateral fringe shift
      of RCP light smoothed using Savitzky-Golay filter in µm ΔY RCP-LCP: The
      dichroic signal fringe shift values in terms of the dispersive part of the
      refractive index in arbitrary units ΔY RCP-LCP: The dichroic signal fringe
      shift values smoothed using Savitzky-Golay filter in terms of the
      dispersive part of the refractive index in arbitrary units ΔY RCP-LCP: The
      dichroic signal fringe shift in terms of the electron scattering factors
      in arbitrary units. B_z: The applied external magnetic field applied in
      the out-of-plane direction with respect to the sample in Gauss. ### File:
      fig2_err.csv Description: The error values of the fringe shift values
      obtained from the registration algorithm for RCP and LCP light. ####
      Variables: LCP error: Error values for the fringe shifts with LCP light.
      RCP error: Error values for the fringe shifts with RCP light. ### File:
      fig3_data.csv Description: The beta values (absorptive part of the
      refractive index) are obtained from the fitting algorithm. These beta
      values are plotted as a function of the beam line energy to show the L2
      and L3 absorptive peaks. The inset shows complementary diode current data
      normalized to absorption. #### Variables: β(RCP): The imaginary part of
      the refractive index for RCP light β(LCP): The imaginary part of the
      refractive index for LCP light β(RCP-LCP): The dichroic signal of
      absorption in terms of imaginary part of the refractive index  Absorption
      (RCP): The diode current normalized to the absorption for RCP light
      Absorption (LCP): The diode current normalized to the absorption for LCP
      light Beamline energy (main panel): The beam line energy scale for the
      main panel 705 to 730 eV Beamline energy (inset panel): The beam line
      energy scale for the inset panel 695 to 735 eV ### File: fig4_data.csv
      Description: The inset displays the results of the registration algorithm
      applied to the beamline energy scans. The main panel presents the first
      derivative of this data with respect to the incident energy, effectively
      resolving the L3 absorption edge peak. #### Variables: ∂ΔY/∂E (LCP): The
      obtained fringe shift values are differentiated with respect to beamline
      energy to obtain the rate of fringe shift for LCP light in µm/eV ∂ΔY/∂E
      (RCP): The obtained fringe shift values are differentiated with respect to
      beamline energy to obtain the rate of fringe shift for RCP light in µm/eV
      ∂ΔY/∂E (RCP-LCP): The obtained dichroic fringe shift values are
      differentiated with respect to beamline energy to obtain the rate of
      fringe shift for the dichroic signal n µm/eV ΔY LCP: Lateral fringe shift
      of LCP light in µm ΔY RCP: Lateral fringe shift of RCP light in µm
      Beamline Energy: The beam line energy scale for both panels from 700 to
      725 eV
    </description>
  </descriptions>
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