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        <formatdesc>Figure 6 shows the ^(31)P{^(23)Na} REAPDOR results for NAGP glass with x = 0. The Fourier transforms of S (top) and Delta S = S_0 - S (bottom) are plotted, where the spectra were obtained for a dipolar mixing time of 1.4 ms. Each spectrum is fitted to two Gaussian peaks.</formatdesc>
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        <formatdesc>Figure 7a shows the ^(31){P^(23)Na} REAPDOR data sets for as-prepared glassy and crystalline NAGP with x = 0.</formatdesc>
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        <formatdesc>Figure 7(b) shows the ^(23){Na^(31)P} REDOR curves for as-prepared glassy and crystalline NAGP with x = 0.  The solid curves show the fits to the NAGP data sets using Eq. 8.</formatdesc>
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        <formatdesc>Figure 8 shows the single-pulse ^{27}Al MAS NMR spectra (black curves) measured for (a) as-prepared glassy, (b) annealed glassy and (c) crystalline NAGP with (I) x = 0.4 or (II) x = 0.8.</formatdesc>
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        <formatdesc>Figure 9 shows the total structure factors S(k) for crystalline NAGP with x = 0, 0.4 and 0.8 measured using GEM [solid (red) curves] or D4c [solid (black) curves].</formatdesc>
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        <formatdesc>Figure 11 shows the total structure factors S(k) for crystalline NAGP with x = 0, 0.4 and 0.8 measured using XRD.</formatdesc>
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        <formatdesc>Figure 12 shows the total structure factors S(k) for as-prepared versus annealed glassy NAGP with x = 0, 0.4 and 0.8 measured using XRD.</formatdesc>
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        <formatdesc>Figure 13 shows the D^prime(r) functions for crystalline NAGP with x = 0 as obtained from the GEM data by the application of either a (a) Lorch or (b) step modification function with k_{max} = 39.1 A^{-1}  and from (c) the XRD data by the application of a step modification function with k_{max} = 24.99 A^{-1}.</formatdesc>
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        <formatdesc>Figure 14 shows the fitted D^prime(r) functions for (a) crystalline and (b) as-prepared glassy NAGP with x = 0 measured using GEM.</formatdesc>
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        <formatdesc>Figure 15 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0 measured using XRD.</formatdesc>
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        <formatdesc>Figure 16 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0 measured using D4c.</formatdesc>
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        <formatdesc>Figure 17 shows the fitted D^prime(r) functions for (a) crystalline and (b) as-prepared glassy NAGP with x = 0.4 measured using GEM.</formatdesc>
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        <formatdesc>Figure 18 shows the fitted D^prime(r) functions for (a) crystalline and (b) as-prepared glassy NAGP with x = 0.8 measured using GEM.</formatdesc>
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        <formatdesc>Figure 19 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0.4 measured using XRD.</formatdesc>
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        <formatdesc>Figure 20 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0.8 measured using XRD.</formatdesc>
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        <formatdesc>Figure 21 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0.4 measured using D4c.</formatdesc>
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        <formatdesc>Figure 22 shows the fitted D^prime(r) functions for (a) crystalline, (b) as-prepared glassy and (c) annealed glassy NAGP with x = 0.8 measured using D4c.</formatdesc>
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        <formatdesc>Figure 23 shows the composition dependence of the (a) electrical conductivity sigma at 573 K and (b) activation energy E_a in crystalline versus as-prepared glassy NAGP  (Ortiz-Mosquera et al. 2019, Zhang et al. 2009}, and (c)-(e) several of the parameters describing the NBO atoms in as-prepared versus annealed NAGP glasses.</formatdesc>
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        <formatdesc>Figure 5 shows the single-pulse ^{31}P MAS NMR spectra measured for the NAGP materials with x = 0: (a) as-prepared glass; (b) glass annealed at T_{TT} = 873 K for 0.25 h; (c) glass annealed at T_{TT} = 876~K for 0.5 h; (d) crystalline material.</formatdesc>
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        <formatdesc>Figure S1 shows the single-pulse ^{31}P MAS NMR spectra (black curves) measured for (a) as-prepared glassy, (b) annealed glassy (T_{TT} = 873 K) and (c) crystalline NAGP with x = 0.</formatdesc>
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        <formatdesc>Figure S2 shows the fitted D^prime(r) functions measured using D4c for NAGP with x = 0 annealed at T_{TT} = 876 K for either (a) 0.25 h or (b) 0.5 h.</formatdesc>
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        <formatdesc>Figure 10 shows the total structure factors S(k) for as-prepared versus annealed glassy NAGP with x = 0, 0.4 and 0.8. The red curves give the GEM data sets and the black or blue curves give the D4c data sets, where the latter correspond to the x = 0 glass annealed at T_{TT} = 876~K for either 0.25 or 0.5~h.</formatdesc>
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          <family>Salmon</family>
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    <title>Data sets for &quot;Structure of crystalline and amorphous materials in the NASICON system Na_{1+x}Al_xGe_{2-x}(PO_4)_3&quot;</title>
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    <abstract>Data sets used to prepare Figures 5-23 and Figures S1-S2 in the Journal of Chemical Physics article entitled &quot;Structure of crystalline and amorphous materials in the NASICON system Na_{1+x}Al_xGe_{2-x}(PO_4)_3 .&quot;  The data sets refer to the measured structure of these materials for the compositions x = 0, 0.4 and 0.8. NASICON is an acronym for sodium (Na) super-ionic conductor.</abstract>
    <date>2021-07-13</date>
    <publisher>University of Bath</publisher>
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        <funder_id>https://doi.org/10.13039/501100000288</funder_id>
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        <project_name>Dorothy Hodgkin Research Fellowship - Rational Design of Glassy Materials with Technological Applications</project_name>
      </item>
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        <funder_name>Engineering and Physical Sciences Research Council</funder_name>
        <funder_id>https://doi.org/10.13039/501100000266</funder_id>
        <grant_id>EP/L015544/1</grant_id>
        <project_name>EPSRC Centre for Doctoral Training in Condensed Matter Physics</project_name>
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        <funder_id>https://doi.org/10.13039/501100000271</funder_id>
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        <project_name>ISIS Facility Development Studentship (Lawrence Gammond)</project_name>
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        <funder_name>Diamond Light Source</funder_name>
        <funder_id>https://doi.org/10.13039/100011889</funder_id>
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        <project_name>ISIS Facility Development Studentship (Lawrence Gammond)</project_name>
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        <funder_name>São Paulo Research Foundation (FAPESP)</funder_name>
        <funder_id>https://doi.org/10.13039/501100001807</funder_id>
        <grant_id>2013/07793-6</grant_id>
        <project_name>Center for Research, Teaching, and Innovation in Glass</project_name>
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        <funder_name>São Paulo Research Foundation (FAPESP)</funder_name>
        <funder_id>https://doi.org/10.13039/501100001807</funder_id>
        <grant_id>2017/17800-0</grant_id>
        <project_name>Postdoctoral Fellowship (Igor d’Anciães Almeida Silva)</project_name>
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    <collection_method>The data sets were collected using the methods described in the published paper.</collection_method>
    <provenance>The data sets were analysed using the methods described in the published paper.</provenance>
    <techinfo>Figures 5 - 8 and S1 were prepared using Origin (http://www.originlab.com/). The data set corresponding to a plotted curve within an Origin file can be identified by clicking on that curve.
Figures 9 - 23 and S2 were prepared using QtGrace (https://sourceforge.net/projects/qtgrace/). The data set corresponding to a plotted curve within an QtGrace file can be identified by clicking on that curve.</techinfo>
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