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        <formatdesc>Figure 1 shows the k-dependence of the singular values sigma_l (l = 1, 2 or 3) and the condition numbers kappa_2  and  kappa_2&apos; for the Faber-Ziman (FZ) (left column) and Bhatia-Thortnon (BT) (right column) partial structure factors.</formatdesc>
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        <formatdesc>Figure 2 shows the temperature dependence of the atomic number density of the melt from experiment and from molecular dynamics simulations.</formatdesc>
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        <formatdesc>Figure 3 shows neutron total structure factors ^{35}F(k) and ^{nat}F(k) and the difference function Delta F(k) measured for NaCl at 1093 K compared to the x-ray total structure factor S_X(k) measured for NaCl at 1091~K. Also shown is the S_X(k) function measured for NaCl at 1083~K in the work of Ohno and Furukawa.</formatdesc>
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      <document id='https://researchdata.bath.ac.uk/id/document/16173'>
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        <formatdesc>Figure 4 shows the Faber-Ziman partial structure factors from the present diffraction work at T = 1093 K, the neutron diffraction work of Biggin and Enderby at T = 1148 K and the polarizable ion model (PIM) simulation at T = 1100 K.</formatdesc>
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        <formatdesc>Figure 5a shows the BT partial structure factor S^{BT}_{NN}(k) from experiment at T = 1100 K and the PIM simulation at T = 1100 K.  Also shown is the breakdown of the simulated function into its contributions from the weighted Faber-Ziman partial structure factors S^{FZ}_{ClCl}(k), S^{FZ}_{NaCl}(k) and S^{FZ}_{NaNa}(k). The inset highlights the measured and simulated BT functions at low-k, plotted as a function of k^2 in order to extract the low-order moments by fitting a straight line.</formatdesc>
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        <formatdesc>Figure 5b shows the BT partial structure factor S^{BT}_{CC}(k) from experiment at T = 1100 K and the PIM simulation at T = 1100 K.  Also shown is the breakdown of the simulated function into its contributions from the weighted Faber-Ziman partial structure factors S^{FZ}_{ClCl}(k), S^{FZ}_{NaCl}(k) and S^{FZ}_{NaNa}(k). The inset highlights the measured and simulated BT functions at low-k, plotted as a function of k^2 in order to extract the low-order moments by fitting a straight line.</formatdesc>
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        <formatdesc>Figure 5b shows the BT partial structure factor S^{BT}_{NC}(k) from experiment at T = 1100 K and the PIM simulation at T = 1100 K.  Also shown is the breakdown of the simulated function into its contributions from the weighted Faber-Ziman partial structure factors S^{FZ}_{ClCl}(k), S^{FZ}_{NaCl}(k) and S^{FZ}_{NaNa}(k). The inset highlights the measured and simulated BT functions at low-k, plotted as a function of k^2 in order to extract the low-order moments by fitting a straight line.</formatdesc>
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      <document id='https://researchdata.bath.ac.uk/id/document/16177'>
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        <formatdesc>Figure 6 shows the partial pair-distribution functions from the present diffraction work at T = 1093 K, the neutron diffraction work of Biggin and Enderby at T = 1148 K and the PIM simulation at T = 1100 K.</formatdesc>
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        <formatdesc>Figure 8 shows the running moments ^{run}M_{IJ}^(0)(r_{max}) from the PIM simulations at T = 1100 K for IJ= NN, CC and NC.</formatdesc>
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        <formatdesc>Figure 9 shows the temperature dependence of the isothermal compressibility.</formatdesc>
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        <formatdesc>Figure 10 shows the Faber-Ziman partial structure factors calculated for molten NaCl at T=1100 K using the PIM, rigid ion model 1 (RIM1) and rigid ion model 2 (RIM2).</formatdesc>
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      <document id='https://researchdata.bath.ac.uk/id/document/16184'>
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        <formatdesc>Figure 11a shows the number-number Bhatia-Thornton partial structure factor calculated for molten NaCl at  T = 1100 K using the PIM, RIM1 and RIM2. Also shown is the function measured in the present diffraction work. The inset zooms into the low-k region of the simulated and measured functions.</formatdesc>
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        <formatdesc>Figure 11b shows the concentration-concentration Bhatia-Thornton partial structure factor calculated for molten NaCl at  T = 1100 K using the PIM, RIM1 and RIM2. Also shown is the function measured in the present diffraction work. The inset zooms into the low-k region of the simulated and measured functions.</formatdesc>
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        <formatdesc>Figure 11c shows the number-concentration Bhatia-Thornton partial structure factor calculated for molten NaCl at  T = 1100 K using the PIM, RIM1 and RIM2. Also shown is the function measured in the present diffraction work.</formatdesc>
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        <formatdesc>Figure 12 shows the total pair correlation functions obtained from the RIM2 simulations at T = 1100 K.</formatdesc>
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        <formatdesc>Figure 13a shows the temperature dependence of the BT total pair-correlation function rh^{BT}_{NN}(r) from the PIM simulations
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        <formatdesc>Figure 13b shows the temperature dependence of the BT total pair-correlation function rh^{BT}_{CC}(r) from the PIM simulations
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        <formatdesc>Figure 13c shows the temperature dependence of the BT total pair-correlation function rh^{BT}_{NC}(r) from the PIM simulations
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        <formatdesc>Figure 14 shows the temperature dependence of the decay length [a_0^{IJ}]^{-1} of Eq.~(42). The values from the PIM simulations at several different temperatures are compared to the values from the diffraction experiment at T = 1093 K.</formatdesc>
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        <formatdesc>Figure 7a shows the Bhatia-Thornton partial pair-distribution function g^{BT}_{NN}(r) from the present diffraction work and from the PIM simulation. Also shown is the breakdown of the simulated function into its contributions from the weighted g_{NaCl}(r), g_{ClCl}(r) and g_{NaNa}(r) functions.</formatdesc>
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        <formatdesc>Figure 7b shows the Bhatia-Thornton partial pair-distribution function g^{BT}_{CC}(r) from the present diffraction work and from the PIM simulation. Also shown is the breakdown of the simulated function into its contributions from the weighted g_{NaCl}(r), g_{ClCl}(r) and g_{NaNa}(r) functions.</formatdesc>
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    <title>Data sets for &quot;Structure of molten NaCl and the decay of the pair-correlations&quot;</title>
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    <abstract>Data sets used to prepare Figure 1 -14 in the Journal of Chemical Physics article entitled &quot;Structure of molten NaCl and the decay of the pair-correlations.&quot; The data sets refer to the measured and simulated structure and thermodynamic properties of molten NaCl.</abstract>
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