From 3cf1cc2ef3ebb0c6427c112942d20ee9eadf18c2 Mon Sep 17 00:00:00 2001
From: Benjamin Regler <regler@fhi-berlin.mpg.de>
Date: Tue, 28 Feb 2017 10:46:26 +0100
Subject: [PATCH] :bookmark: Added periodic table analytics tutorial

---
 beaker-notebooks/periodic-table.bkr           |  841 +++
 .../electronic_affinity_neutral_atoms.json    |  944 +++
 .../data/extended_binaries_dimers_atoms.json  | 2269 +++++++
 .../data/static_polarization.json             | 5782 +++++++++++++++++
 .../periodic-table/data/vdw_coefficients.json | 1674 +++++
 .../periodic-table/periodic_table.min.json    |    1 +
 6 files changed, 11511 insertions(+)
 create mode 100644 beaker-notebooks/periodic-table.bkr
 create mode 100644 example-data/periodic-table/data/electronic_affinity_neutral_atoms.json
 create mode 100644 example-data/periodic-table/data/extended_binaries_dimers_atoms.json
 create mode 100644 example-data/periodic-table/data/static_polarization.json
 create mode 100644 example-data/periodic-table/data/vdw_coefficients.json
 create mode 100644 example-data/periodic-table/periodic_table.min.json

diff --git a/beaker-notebooks/periodic-table.bkr b/beaker-notebooks/periodic-table.bkr
new file mode 100644
index 0000000..bcd6197
--- /dev/null
+++ b/beaker-notebooks/periodic-table.bkr
@@ -0,0 +1,841 @@
+{
+    "beaker": "2",
+    "evaluators": [
+        {
+            "name": "HTML",
+            "plugin": "HTML",
+            "view": {
+                "cm": {
+                    "mode": "htmlmixed"
+                }
+            }
+        },
+        {
+            "name": "JavaScript",
+            "plugin": "JavaScript",
+            "view": {
+                "cm": {
+                    "mode": "javascript",
+                    "background": "#FFE0F0"
+                }
+            },
+            "languageVersion": "ES2015"
+        },
+        {
+            "name": "IPython",
+            "plugin": "IPython",
+            "setup": "%matplotlib inline\nimport numpy\nimport matplotlib\nfrom matplotlib import pylab, mlab, pyplot\nnp = numpy\nplt = pyplot\nfrom IPython.display import display\nfrom IPython.core.pylabtools import figsize, getfigs\nfrom pylab import *\nfrom numpy import *\n",
+            "view": {
+                "cm": {
+                    "mode": "python"
+                }
+            }
+        }
+    ],
+    "cells": [
+        {
+            "id": "load_stylesheets",
+            "type": "code",
+            "evaluator": "HTML",
+            "input": {
+                "body": [
+                    "<style type=\"text/css\">",
+                    "/*!",
+                    " * Nomad Beaker Notebook Template",
+                    " *",
+                    " * @copyright  Copyright 2017 Fritz Haber Institute of the Max Planck Society,",
+                    " *             Benjamin Regler - Apache 2.0 License",
+                    " * @license    http://www.apache.org/licenses/LICENSE-2.0",
+                    " * @author     Benjamin Regler",
+                    " * @version    1.0.0",
+                    " *",
+                    " * Licensed under the Apache License, Version 2.0 (the \"License\");",
+                    " * you may not use this file except in compliance with the License.",
+                    " * You may obtain a copy of the License at",
+                    " * ",
+                    " *     http://www.apache.org/licenses/LICENSE-2.0",
+                    " *",
+                    " * Unless required by applicable law or agreed to in writing, software",
+                    " * distributed under the License is distributed on an \"AS IS\" BASIS,",
+                    " * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.",
+                    " * See the License for the specific language governing permissions and",
+                    " * limitations under the License.",
+                    " */",
+                    "p{margin-bottom:1.3em}h1,h2,h3,h4{margin:1.414em 0 .5em;font-weight:inherit;line-height:1.2}h1{margin-top:0;font-size:3.998em}h2{font-size:2.827em}h3{font-size:1.999em}h4{font-size:1.414em}.font_small,small{font-size:.707em}.notebook-container{font-size:16px}.notebook-container .bkr{font-size:100%;font-weight:400;line-height:1.45;color:#333}.nomad--header h2{color:#20335d;font-weight:700;margin:0 0 .2em}.nomad--header h3{color:#20335d;font-weight:700;margin-top:0;text-indent:-1em;padding-left:1em}.nomad--header h3:before{content:\"\\2014\";padding-right:.25em}.nomad--header .nomad--description{margin:-1em 0 0 2em}.atomic-data--block,.nomad--last-updated{display:inline-block;margin-top:1em}.nomad--last-updated{color:grey;float:right;position:relative;z-index:1}.nomad--last-updated::before{bottom:-75%;content:attr(data-version);font-size:4em;font-weight:700;opacity:.2;position:absolute;right:0}.atomic-data label{display:block;font-size:medium;font-weight:700}.atomic-data--select,.chosen-container{width:100%!important}.atomic-data--select:disabled{color:#d3d3d3}.atomic-data--reset-buton{display:inline-block;margin-top:1.6em;width:100%}.modal-dialog{max-width:1000px;width:80%}.modal-header h1{font-size:2em;line-height:1.2}.modal-dialog h2{font-size:1.414em}.modal-dialog h2:first-child{margin-top:0}.modal-dialog h3{font-size:1.2em}.modal-dialog dt{font-size:larger;margin-top:1.414em}.modal-dialog img{width:100%}.modal-dialog .authors{text-transform:uppercase}",
+                    "/*!",
+                    " * Periodic Table",
+                    " *",
+                    " * @copyright Copyright 2017 Benjamin Regler - MIT License",
+                    " * @license   https://opensource.org/licenses/MIT",
+                    " * @author    Benjamin Regler",
+                    " * @version   1.0.0",
+                    " */",
+                    ".periodic-table{margin-bottom:2em}.periodic-table--header{text-align:center}.periodic-table--title{margin:0}.periodic-table--description{margin:0 0 2em}.periodic-table--credits{font-size:x-small;text-align:right}.periodic-table--colormap{margin-bottom:1em}.periodic-table--colormap-canvas{background-color:#5bc0de;cursor:crosshair;height:1em;width:50%}.periodic-table--colormap-value{display:inline-block;vertical-align:bottom;padding:0 .2em;position:relative;min-width:2em}.periodic-table--colormap-value::before{font-size:smaller;font-weight:700;position:absolute;top:100%}.periodic-table--colormap-value.min{text-align:right}.periodic-table--colormap-value.min::before{content:\"Min\";right:0}.periodic-table--colormap-value.max::before{content:\"Max\"}#periodic-table--colormap-1__hover{background-color:#fff;border:1px dotted #000;display:none;font-size:small;padding:.2em;position:absolute;z-index:10000}#periodic-table--colormap-1__hover 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+                    " * Atomic Data",
+                    " *",
+                    " * @copyright  Copyright 2017 Fritz Haber Institute of the Max Planck Society,",
+                    " *             Benjamin Regler - Apache 2.0 License",
+                    " * @license    http://www.apache.org/licenses/LICENSE-2.0",
+                    " * @author     Benjamin Regler",
+                    " * @version    1.0.0",
+                    " *",
+                    " * Licensed under the Apache License, Version 2.0 (the \"License\");",
+                    " * you may not use this file except in compliance with the License.",
+                    " * You may obtain a copy of the License at",
+                    " * ",
+                    " *     http://www.apache.org/licenses/LICENSE-2.0",
+                    " *",
+                    " * Unless required by applicable law or agreed to in writing, software",
+                    " * distributed under the License is distributed on an \"AS IS\" BASIS,",
+                    " * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.",
+                    " * See the License for the specific language governing permissions and",
+                    " * limitations under the License.",
+                    " */",
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+                    "</style>"
+                ],
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+                "body": [
+                    "<div class=\"nomad--header\">",
+                    "    <h2>NOMAD Analytics Toolkit</h2>",
+                    "    <h3>A Periodic Table Of Elements for Atomic Data Collections</h3>",
+                    "    <p class=\"nomad--description\">",
+                    "        created by <a href=\"mailto:regler@fhi-berlin.mpg.de\">Benjamin Regler</a> (Fritz Haber Institute of the Max Planck Society, Faradayweg 4-6, D-14195 Berlin, Germany).",
+                    "        <span class=\"nomad--last-updated\" data-version=\"v1.0.1\">[Last updated: February 28, 2017]</span>",
+                    "    </p>",
+                    "</div>"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "state": {},
+                "result": {
+                    "type": "BeakerDisplay",
+                    "innertype": "Html",
+                    "object": "<script>\nvar beaker = bkHelper.getBeakerObject().beakerObj;\n</script>\n<div class=\"nomad--header\">\n    <h2>NOMAD Analytics Toolkit</h2>\n    <h3>A Periodic Table Of Elements for Atomic Data Collections</h3>\n    <p class=\"nomad--description\">\n        created by <a href=\"mailto:regler@fhi-berlin.mpg.de\">Benjamin Regler</a> (Fritz Haber Institute of the Max Planck Society, Faradayweg 4-6, D-14195 Berlin, Germany).\n        <span class=\"nomad--last-updated\" data-version=\"v1.0.1\">[Last updated: February 28, 2017]</span>\n    </p>\n</div>"
+                },
+                "selectedType": "BeakerDisplay",
+                "elapsedTime": 1,
+                "height": 161
+            },
+            "evaluatorReader": true,
+            "lineCount": 8
+        },
+        {
+            "id": "markdownxSre89",
+            "type": "markdown",
+            "body": [
+                "### Introduction",
+                "",
+                "The periodic table of elements structures chemical elements according to similar, and recurring, chemical properties and gives useful information about their structure (see [Dimitri Mendeleev](https://en.wikipedia.org/wiki/Dmitri_Mendeleev)). It is used by [Nomad laboratory](https://www.nomad-coe.eu/) to visualize atomic data collections. Atomic data collections are data sets of atomic properties. They are enhanced by metadata attributes from where the data come from, how they were generated or measured, and what settings have been used. Atomic properties are the radius, the atomic mass, but also the ionization potential, the expectation values of the orbitals, and many other properties that describe the elements.",
+                "",
+                "Atomic data collections are often created with a purpose and an actual application in mind. In most cases, they are subsets of available atomic properties within the periodic table of elements. They are usually used for, e.g, data mining programs to provide initial data (e.g., control parameters and physical properties used as input variables), to derive quantitative statements about the interpretation of outcomes, and to make predictions about future probabilities or trends for a chosen set of observables (output variables).",
+                "",
+                "In this notebook, we use the Nomad infrastructure to query a limited number of atomic data collections and to visualize them in the periodic table of elements. There are several filters that can be applied to atomic data collections and a field to select which atomic property should be visualized in the periodic table of elements. Please check out the usage instructions for more details or go ahead and scroll down to the viewer."
+            ],
+            "evaluatorReader": false
+        },
+        {
+            "id": "codeBI4ymq",
+            "type": "code",
+            "evaluator": "HTML",
+            "input": {
+                "body": [
+                    "<button type=\"button\" class=\"btn btn-info\" data-toggle=\"modal\" data-target=\"#modal-instructions\" style=\"font-size:larger;\">Read usage instructions</button>",
+                    "<div class=\"modal fade\" id=\"modal-instructions\" tabindex=\"-1\" role=\"dialog\" aria-labelledby=\"modal-instructions\">",
+                    "  <div class=\"modal-dialog\" role=\"document\">",
+                    "    <div class=\"modal-content\">",
+                    "      <div class=\"modal-header\">",
+                    "        <button type=\"button\" class=\"close\" data-dismiss=\"modal\" aria-label=\"Close\"><span aria-hidden=\"true\">×</span></button>",
+                    "        <h1 class=\"modal-title\" id=\"modal-instructions-label\">Usage instructions</h1>",
+                    "        <hr>",
+                    "      </div>",
+                    "      <div class=\"modal-body modal-instructions-body\">",
+                    "        <h2>Introduction</h2>",
+                    "",
+                    "        <p>This notebook provides a selected and curated list of atomic data collections to be visualized in the periodic table of elements.</p>",
+                    "",
+                    "        <p>Atomic data collections are data sets of atomic properties. They are enhanced by metadata attributes from where the data come from, how they were generated or measured, and what settings have been used. Atomic properties are the radius, the atomic mass, but also the ionization potential, the expectation values of the orbitals, and many other properties that describe the elements.</p>",
+                    "",
+                    "        <h2>Visualization</h2>",
+                    "",
+                    "        <h3>Atomic data collections:</h3>",
+                    "",
+                    "        <p>Multiple atomic data collections can be selected for the visualization. Their are shown and sorted according to their atomic data collection name. Additional information will be shown once the mouse cursor hovers over the name. You can select multiple atomic data collections, where the order specifies the priority of the collections, i.e., when two or more collections have the same atomic properties. In this case collections that are selected first have higher priority than collections that are selected last and overwrite those values if present.</p>",
+                    "",
+                    "        <img 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\" />",
+                    "",
+                    "        <h3>Filters:</h3>",
+                    "",
+                    "        <p>There exist several filters to select only a specific subset of atomic data collections. Filters are only available once an atomic collection is selected and filters that are not available are disabled. You can add as many filters as selection criteria as you want.</p>",
+                    "",
+                    "        <img src=\"data:image/png;base64,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/>",
+                    "        ",
+                    "        <p>Please note that the order is important here as well. For example, consider the atomic data collection has experimental and theoretical data and if you select <code>Theory, Experiment</code>, then all data are shown, but theoretical values overwrite experimental values when present.</p>",
+                    "",
+                    "        <h3>Atomic properties:</h3>",
+                    "",
+                    "        <p>Once an atomic data collection has been set and an optional selection filter criteria has been applied, it is possible to visualize the atomic properties in the periodic table of elements. The elements will be colored by the value of the selected atomic property. A colormap shows the range of the atomic property value (including the minimum and maximum value). For an empty value, all available atomic properties in the table will be displayed. Elements that are shown in gray are not in the set of atomic collections or have been filtered out by the selection criteria. For all other elements, additional information is provided when the mouse cursor hovers over the element.</p>",
+                    "      ",
+                    "        <p>The visualization resets, when the set of atomic data collections or the selection criteria changes and updates when an atomic property is selected again.</p>",
+                    "",
+                    "        <img 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\" />",
+                    "      </div>",
+                    "      <div class=\"modal-footer\">",
+                    "        <button type=\"button\" class=\"btn btn-default\" data-dismiss=\"modal\" style=\"font-size:larger;\">Close</button>",
+                    "      </div>",
+                    "    </div>",
+                    "  </div>",
+                    "</div>",
+                    "",
+                    "<button type=\"button\" class=\"btn btn-default\" data-toggle=\"modal\" data-target=\"#modal-credits\" style=\"font-size:larger;\">Credits</button>",
+                    "<div class=\"modal fade\" id=\"modal-credits\" tabindex=\"-1\" role=\"dialog\" aria-labelledby=\"modal-credits\">",
+                    "  <div class=\"modal-dialog\" role=\"document\">",
+                    "    <div class=\"modal-content\">",
+                    "      <div class=\"modal-header\">",
+                    "        <button type=\"button\" class=\"close\" data-dismiss=\"modal\" aria-label=\"Close\"><span aria-hidden=\"true\">×</span></button>",
+                    "        <h1 class=\"modal-title\" id=\"modal-credits-label\">Credits</h1>",
+                    "        <hr>",
+                    "      </div>",
+                    "      <div class=\"modal-body modal-credits-body\">",
+                    "        <h2>Atomic Data:</h2>",
+                    "",
+                    "        <p>This notebook is based on the NOMAD Atomic Data Parser and Interface written by <a href=\"mailto:regler@fhi-berlin.mpg.de\">Benjamin Regler</a>.</p>",
+                    "        <ul>",
+                    "          <li><span class=\"authors\">Regler, B.</span>: <em>NOMAD Atomic Data Parser and Interface</em>. Fritz Haber Institute of the Max Planck Society, Germany (2017).</li>",
+                    "        </ul>",
+                    "",
+                    "        <h2>Atomic Data Collections:</h2>",
+                    "        <dl>",
+                    "          <dt>Experimental and theoretically derived values for isotropic static polarizability</dt>",
+                    "          <dd>",
+                    "            <p>This collection includes experimental and theoretically derived values for isotropic static polarizability as complied by <a href=\"http://ctcp.massey.ac.nz/?group=schwerd\">Prof. Peter Schwerdtfeger</a>.</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Schwerdtfeger, P.</span>: <em>Table of experimental and calculated static dipole polarizabilities for the electronic ground states of the neutral elements (in atomic units)</em>. Centre for Theoretical Chemistry and Physics, The New Zealand Institute for Advanced Study (2014). [<a href=\"http://ctcp.massey.ac.nz/Tablepol2014.pdf\">link</a>]</li>",
+                    "            </ul>",
+                    "            <p>Not all published values are compiled, only the most accurate ones. There is some confusion about the experimental data listed in the <a href=\"https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286\">CRC Handbook of Chemistry and Physics</a> taken from Miller and Bederson. Some of the data are not experimental values as indicated, but from LDA calculations of Doolen, which are listed here as well.</p>",
+                    "            <p>A more recent review by Mitroy, Safronova and Clark is highly recommended:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Mitroy, J.; Safronova, M. S. &amp; Clark, C. W</span>: <em>Theory and applications of atomic and ionic polarizabilities</em>. Journal of Physics B: Atomic, Molecular and Optical Physics <strong>43</strong>, 202001 (2010). DOI: <a href=\"https://dx.doi.org/10.1088/0953-4075/43/20/202001\">10.1088/0953-4075/43/20/202001</a>.</li>",
+                    "            </ul>",
+                    "          </dd>",
+                    "",
+                    "          <dt>Experimental electron affinities for neutral atoms</dt>",
+                    "          <dd>",
+                    "            <p>The values for experimental electron affinity for neutral atoms are taken from</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Lide, D. R.</span>: <em>CRC Handbook of Chemistry and Physics 86th ed.</em>. CRC Press, 2616 pp. (2005). [<a href=\"https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286\">link</a>]</li>",
+                    "            </ul>",
+                    "          </dd>",
+                    "",
+                    "          <dt>Extended binaries, dimers and atoms</dt>",
+                    "          <dd>",
+                    "            <p>This collection provides data for extended binaries, dimers, and atoms. It contains atom property information for rock-salt and zincblende crystal lattice structures, octet (I/II/III)-(V/VI/VII) binary materials, other eight-electron binaries using possible valences of d-metals and f-elements, and octet binaries from John and Bloch's paper:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">John, J. &amp; Bloch, A. N.</span>: <em>Quantum-Defect Electronegativity Scale for Nontransition Elements</em>. Physical Review Letters, American Physical Society, <strong>33</strong>, 1095-1098 (1974). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.33.1095\">10.1103/PhysRevLett.33.1095</a>.</li>",
+                    "            </ul>",
+                    "            <p>The atomic properties in this collection are obtained from:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Ghiringhelli, L. M.; Vybiral, J.; Levchenko, S. V.; Draxl, C. &amp; Scheffler</span>: <em>M. Big Data of Materials Science: Critical Role of the Descriptor</em>. Physical Review Letters, American Physical Society <strong>114</strong>, 105503 (2015). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.114.105503\">10.1103/PhysRevLett.114.105503</a>.</li>",
+                    "            </ul>",
+                    "          </dd>",
+                    "        ",
+                    "          <dt>Isotropic static polarizabilities and homo-atomic van der Waals coefficients for neutral free atoms</dt>",
+                    "          <dd>",
+                    "            <p>The majority of values such as isotropic static polarizability (in bohr<sup>3</sup>) and the homo-atomic van der Waals coefficient (in hartree &middot; bohr<sup>6</sup>) for neutral free atoms are taken from:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Chu, X. &amp; Dalgarno, A.</span>: <em>Linear response time-dependent density functional theory for van der Waals coefficients</em>. The Journal of Chemical Physics <strong>121</strong>, 9, 4083 (2004). DOI: <a href=\"https://dx.doi.org/10.1063/1.1779576\">10.1063/1.1779576</a>.</li>",
+                    "              ",
+                    "              <li><span class=\"authors\">Mitroy, J.; Safronova, M. S. &amp; Clark, C. W</span>: <em>Theory and applications of atomic and ionic polarizabilities</em>. Journal of Physics B: Atomic, Molecular and Optical Physics <strong>43</strong>, 202001 (2010). DOI: <a href=\"https://dx.doi.org/10.1088/0953-4075/43/20/202001\">10.1088/0953-4075/43/20/202001</a>.</li>",
+                    "            </ul>",
+                    "            <p>The rest of the elements are calculated using linear response coupled cluster single double theory with accurate basis. The van der Waals radii for the respective elements are defined as discussed in:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Tkatchenko, A. &amp; Scheffler</span>: <em>Accurate Molecular Van Der Waals Interactions from Ground-State Electron Density and Free-Atom Reference Data</em>. Physical Review Letters <strong>102</strong>, 073005 (2009). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.102.073005\">10.1103/PhysRevLett.102.073005</a>.</li>",
+                    "            </ul>",
+                    "            <p>For lanthanides and actinides, the C<sub>6</sub> coefficients are constructed to satisfy the valence electronic sum rule using the one-term formula which is equivalent to the two-point zeroth-order Pad&eacute; approximant. Here, static polarizabilities are taken from:</p>",
+                    "            <ul>",
+                    "              <li><span class=\"authors\">Dzuba, V. A.; Kozlov, A.; Flambaum; V. V.</span>: <em>Scalar Static Polarizabilities of Lanthanides and Actinides</em>. Physical Review A <strong>89</strong>, 042507 (2014). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevA.89.042507\">10.1103/PhysRevA.89.042507</a>.</li>",
+                    "            </ul>",
+                    "          </dd>",
+                    "        </dl>",
+                    "      </div>",
+                    "      <div class=\"modal-footer\">",
+                    "        <button type=\"button\" class=\"btn btn-default\" data-dismiss=\"modal\" style=\"font-size:larger;\">Close</button>",
+                    "      </div>",
+                    "    </div>",
+                    "  </div>",
+                    "</div>",
+                    "",
+                    "<p></p>"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "state": {},
+                "result": {
+                    "type": "BeakerDisplay",
+                    "innertype": "Html",
+                    "object": "<script>\nvar beaker = bkHelper.getBeakerObject().beakerObj;\n</script>\n<button type=\"button\" class=\"btn btn-info\" data-toggle=\"modal\" data-target=\"#modal-instructions\" style=\"font-size:larger;\">Read usage instructions</button>\n<div class=\"modal fade\" id=\"modal-instructions\" tabindex=\"-1\" role=\"dialog\" aria-labelledby=\"modal-instructions\">\n  <div class=\"modal-dialog\" role=\"document\">\n    <div class=\"modal-content\">\n      <div class=\"modal-header\">\n        <button type=\"button\" class=\"close\" data-dismiss=\"modal\" aria-label=\"Close\"><span aria-hidden=\"true\">×</span></button>\n        <h1 class=\"modal-title\" id=\"modal-instructions-label\">Usage instructions</h1>\n        <hr>\n      </div>\n      <div class=\"modal-body modal-instructions-body\">\n        <h2>Introduction</h2>\n\n        <p>This notebook provides a selected and curated list of atomic data collections to be visualized in the periodic table of elements.</p>\n\n        <p>Atomic data collections are data sets of atomic properties. They are enhanced by metadata attributes from where the data come from, how they were generated or measured, and what settings have been used. Atomic properties are the radius, the atomic mass, but also the ionization potential, the expectation values of the orbitals, and many other properties that describe the elements.</p>\n\n        <h2>Visualization</h2>\n\n        <h3>Atomic data collections:</h3>\n\n        <p>Multiple atomic data collections can be selected for the visualization. Their are shown and sorted according to their atomic data collection name. Additional information will be shown once the mouse cursor hovers over the name. You can select multiple atomic data collections, where the order specifies the priority of the collections, i.e., when two or more collections have the same atomic properties. In this case collections that are selected first have higher priority than collections that are selected last and overwrite those values if present.</p>\n\n        <img 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\">\n\n        <h3>Filters:</h3>\n\n        <p>There exist several filters to select only a specific subset of atomic data collections. Filters are only available once an atomic collection is selected and filters that are not available are disabled. You can add as many filters as selection criteria as you want.</p>\n\n        <img 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       \n        <p>Please note that the order is important here as well. For example, consider the atomic data collection has experimental and theoretical data and if you select <code>Theory, Experiment</code>, then all data are shown, but theoretical values overwrite experimental values when present.</p>\n\n        <h3>Atomic properties:</h3>\n\n        <p>Once an atomic data collection has been set and an optional selection filter criteria has been applied, it is possible to visualize the atomic properties in the periodic table of elements. The elements will be colored by the value of the selected atomic property. A colormap shows the range of the atomic property value (including the minimum and maximum value). For an empty value, all available atomic properties in the table will be displayed. Elements that are shown in gray are not in the set of atomic collections or have been filtered out by the selection criteria. For all other elements, additional information is provided when the mouse cursor hovers over the element.</p>\n      \n        <p>The visualization resets, when the set of atomic data collections or the selection criteria changes and updates when an atomic property is selected again.</p>\n\n        <img 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Ups6UvPlConyAKDRU6431xz2gsUEHu4srGeh3A6p/nIGL51VILHzuA83a0v49kh5l5szdKdxC8VpXMQJ9UKruEDkuVntD16Q+xiB45zOlPKOetfvSyXpjwppvm8P7dp3soD2jjB2MtKWaKiQAt81Kp2M6CLzWCdzxAmFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQqBGp+HRzJp0CsPnhFccrh2btCDhdXjR9B5/v1r5olaSXcqkeId96iV8AQVF2Jrs8nYPSz1+GDxO4/E2LZqN/KKQzIqoTFmZrVnww3/WyUShnaSpXfaND2SrJWMstcbIvOjo4+U4WygvMUxaYVSFfghhxQo0FThuPJZ7dWWFSq42qleR52h1xsi/acIxphyQ9ZHf+ui0MOPmO04/w8NDZ09ShjqjkbkxMvHc0VfuJ+VpB7Ip3o4JTyqMKvLDxpMRpk4jkHGEJnj9URNzh5KIoreoWAI8IJygi7SqTPwq/mgKdB974obKNV/AeFZzWFuJ1wiczTvQaBc9fA2ScXCmsOKWvkaTdXvW+uBjXGmlfKuKEGnOcaIC23xuxOEEJFZziAklcKhJxQo0PTlADDlOcghcqIG6qZxf+pTV7U/ARtPF300snKryJMkfLFAJ+ZE2Wy4UcJ03R9AusXWaSOdTg9OTeZZqA+44XYjg1nC6UAvVNXmOV122elkBN/aWPdmuyDlo47XAK+eg8MVh/hTaGmmE5ygc2K9lMP2YuDzGFGMv0k8Bn+6YMq9vkw4m2PHjaq4jXlP3r6aMMLSNKmTyRDUy5r2TLDDgV79Bm0cxx8q1X3s3iNYrTvUz+xM1UfZXXb57WFnXMZNLtGC5OoR9dJAsDGyrFNYW+TrUoeVykFem18/Q4ZYtP8vzej4ognLIlfk1E+qV7+3wFrwuspgce7ry8WcOIpszBzXJjJXDo9u17FUacaNG8Q7cT7xXst3GnWinv4bHbifRCWZsVvB4mJp6Gf+yC90qVN2yeoqwCaWOq7iHgm3L7doV08DYo1Q1OoR89kBl4yB7XF0obE2//kCnJVzAOKQlP/DXxXiGHpvv2o0zpJqy3le/Qh7BrTmdiOn4S4RTcw+5WiW9ReBjI4DV7Y66wIJmRKvEtTd/CnoEn9uWLeqbHCV45zIIc3xSbtlN6q9J82yRwCrDKdzKTZ+aUKm/YPEXFIlIlSl6FgTmstpPJR2cbSIHgVFdJ/BrHZiXZaWtweJ5JVNtOsGV8V8xFc5o8ONHTNgfZVUo35suxH1Qh+sUrV1uZESgjss+i1qqRVroBJ1p0s/tUBFS93QInXgVp2JShqfLGzVOb/vTaxLo8nw1OyunjrcRm2awBJn8n8FfA9OhazEoq28sXquIEW4ZJicmF096vLnzBDUGtpSkVtOpok2wyI2sLlWbAelbbgYKvvaY4rS3U1XInnKC67uI48UrJto9uj1zljZuntRjtw+AafuZpODiZfHSxFWIjFPO1Lkk/U0aIO7lPdqIiHielctFwBR7vXsD0ZAcNn8xw0re3dmufMOKUbXcuy9SddhFdolyQKld54+ZZuVPQ1p2gVcaVr8XJ+qMrBiMWZ7OTsiXJgBNtV9ZfwUBvcuEkrptdq+1LZ+FOtZKSWebf0+oTRpw0RW1xCl443SxSe3qcYEGHNTgZN0/XdkoNTfQNp+1k/dEVNsTibHZSKE6kmJ4oyDuUj5VtUuB089ixRJqCkpvjqvab41SlNqd4O1t9wohTlT5hYIWTnIY2xylVrfLGzTOk8tRUhHg4HJysP7oRJ5udZIITqaPn7aRAEzrUJMrsybk1ff135U5Vz+lOxQU0l7x4QVxloZzZk1cqGv+qg1jgCSuWmy9iu9h2DM+drD56qDtZ7iQznOhJ7i8kuy8W1AuKk/GxU9spk9pJrWXbqdZV20lJoRWH4CTSHpr2jfnyRD8IddH80XBwsv7oRpxsdpI5Tnz0yD7MSEw2nDRZO0ucNOk67ktQIcWbUkaS2VO7fQNOGfqVVvHt02TfLPoWZGdq+o6n7BhBnz3rj27EyWYnWeFEP6TTYDHUC4eT8USRGU70bNNWbYufNly2yVVzn+68U4UuBjPHKbhGebtkwEk+Has5N2RxHgs2Re4BxE4vfz3sHuXWH92Ik81O0uC0m1jZPGqy4KR2cCBZuRY4KWXk05f0ZOv+VF4j9TipnSqCrXbuxNsVNAemwyld7nbBg8rQzdNTId3kXTPuK+OdXOK02/6jG3Gy2UkyTppTca3K9xQm9yYdTpSIwMPE2/dOs7DNFCfREU/ts7eWdruG9xRIzXqcWJYhwPrshY5NVNpOUKEDRxd/9ahQylQ6GdUfYsuTNsp9dvISE79JNW6e9uufj8Y9y0fjyqkRU5w2yqNx/5pvs2wbnKx3kowTDTcP3b53eTM0H+t3JrLejLswtTfpcFI7S7MvYFOcQnqU+47L/b+fFLDuN2pRJQceOrYppEd54Mh6bhRqD3PRX5CeC+WjhfWbZ2ztG+eKsO8VoZybMl22DU7WO0nGSf5ImzS9y9GcJiFO8lCeh41eq2CPlZF0453YmJ76Jm/6GlZcU7TuERQN1B/Ktc7sAQkV/ERyNg+RfD/eMwySyjoND2+WGTfP0H46T18KfKfOZOQGJ6tl2+FkuZNknEg67X5efzSfnqGmmNd/g96EQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFGr8NNdrMsE5CoUagVJON67fjYOFUBGv9PuSYQYRl/Lt2Ri2safZB29XHPE+xyp9e772Pvde8B0vlALfFVmvLztwZAdewQllV5MDTYvXWb983LL6+I4fGvmkcobFri08skOZF2IkqzTF6bj7qs/2QnbmkQVf3c43rE+zlKwdu3/Auf1RNqq1nXzHt/7waHwb2y12RKs0w2k4C2J7odbssvbapWRdLvrhCFYZlHU1ZNMp0FkP6pvoRAk7C9jkDr7jFZK0sYjObCcdzFdfPvRFZuDo8WapvpGQ9ftS2XQJeWzmBHitQgocTRXL0LyFP03EM+xlOlfLwfs0klrbvFWxguGukq2Wl+M4KW+iRY6wBS0wbs3pTDG3mGadfC+sETOpaEqt37d3h2ZTN7SQOKwzKGvNrTqYm+zbc/DKVz8AR+lrDjYu4BOjLFvwZMfX3r17DpdpX85r9FVJ+/LT78NXNtRt3568K4t/zOU45TWSysLdfBm6t7CnoR1yZfEPQC59eTld7Fp66csqZdqU4a+St27YUhlO6gNWhC3IuDWBJm9DgTITjbxOthfoTVxWxSZNKVjfXpNNRaFswpxiWnXS1+z3pq/RTBQHYU4qC3U0L0M7Ym0hrVrwdQ11rVitmew1357DqWwZ+rfQp4sL2JWsM9jLbLHpa76Gl3cbIqthrJLQOf74UhlO8gNRRKzEZGu+9hrWKQd7+SRlxyailqL4WmwqCmWB01o6K7IP6o6KUyWdGVLUbf3LxYUb+LvgibXqdMr8rVDn2R3DEuHptXyaPg1OpDZvc/Ff1PmYh71Kwq5yxpbKKr/8QBRRcdIvTYuTWKcRp10GnIybikINB6eGwv1ltCINEyff+o2pZhUYnpaLanCCwKpWDaCGv0qKk3jEcRIP3OMkr9MRJ/2molDOwd7XarBXm7eNVSgWCelf1tZtXbC3y6sppHsLvSMXlXFiExXvu68GUMNfJQv2Nqk4yQ/UYC+VmGyNBid5nfY4hWwqCmWDE2u7P2JNdYFTduaR5OOF1CoOFn0Vp3tZW7eDe/KaFvzYyDHZ1/rkB7ABURmVt4infazoN7JdwWJboE2ksZrhr5JhxJfq27NxcZn8QBRhC1pu2Bo9TvI6bXEK3VQUygYnkWH2qjj5HhVKDy9AeNNQINVv1r2srdsk5T7PQFOcAhJLZvNlqG8RT/MpiI+KeJItlgTXaAKo4a+SqEsllYWBTcoDUYQuqMiwNXqclHVa42S2qSjUKEuXFHR8Wry4Y1PEfLzI2VTU5MSp7pFZN4QJqQjaVNTkxMm3J9A00rWl8GvgjPRySsN9+/NsKgo10eVbwFQ2Pm9HoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAoFAqFQo1IWfd27rziHfbbUv6a6rqgq7K8nIuiKX9dfr6IEP+FRqeSQZfllIJOa9eUc/35yTCWGKaFDu8Ihf0AjcIRCvsBGq39nnLvm8U/7iyKKJxSK7/xkvRj+Y7LdFtOLui4drVcuI6AbokvDE5hP0JhP0CjtN8rD8GSksjJnTt3FqWf33mo8WST/2QTPDyU73iwUs4WuT5ajmWVD1Z5KPFYkX1BegAammKdShK35eSCjmtXy7nYUFfSLTFcC1UqtZuFuV2vWvOcjqV6hByLDrOc49p1u9OuqHG/u6vMTvJfOOpdu3PnBg7RN96GQxfYvabgo62OOFXe/sbrFifHsmqFaiTFsIPtCoJL+8CtnUoSt+Xkgo5rV8u52FCXB0CzxHAtVMHJzcLcrleteU7HUj1CjkWHWc5x7brdaVfUuN/dVWYX7lTme3JvA7WjXIhh048lyu5U5vgNlFh2vsglTs5ltd/PZxsdQC7+5sk3sAccShLX5URB57Ur5VxsqDtplxi2haru5Lwwt+tVNtHxWKpHyPmwD6+c89q1u9O2qGG/u6vMTornbSdwp4azuSe/aQF3+mb+BXgY6+pg3XMmWjla9xy/0pTvyXS7WJYerOD5RDj2TiWJ63KioPPalXIuNtRtMkJdYtgWqrqT88LcrldLvP2x1Bwhx8M+vHLOa9cdILuixv3uqjK7y+x9U0aDvW/20rZTyj3wKTc4LT+fC9uU6wonF2W1HyzxSqxDE7uSNu2cShL35XhBF2uXy7ko6jo+yB/Gpx+uOzkvzO165U10PpbKEQq6qCLDKeem1qm706Gobr+7rMwu/ImgUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUCoVCoVAo1KiowWWXwfTzx4656yQdPH/sr277TaUcc1Uy+OjsWXfb6fvx2DF3veUqz549e2ibq7VfOOZyMy+4/OR0p/tcLZUdHlfHiBZydZBoQXfHiK83xeVmujtI7KO7OUi0oLtjxFbu9hiNqnw/nj3qDqfKptiUY2UuS7pn9KyrfeB+oCWsOX2Zyz7FvgvuwINlFrv6QJVNXjdbync6LDXLaamspKtjxAu5OEhKwQZXK3d1jHjJYX10p4Mkf2jnY6QssjgcfcmfE6fFWS43wh8L+6vM5WIr3Y2d811odNf/t+Gsy699/8nERNffUsXfuBw4/k2qq+8HPxtqts3dTvefbHQeEM5KujpGvJCLg6QszfEY8ZJujhEv6eYgiY/ufJDkzXQ+Rryk22M02nLPdPp5lyPifBdcDjGuvOKyO31dqzfrr/lucLpwtCXLpZX5Lrj8PHvvnXX3gSrhK9KV3cJO91/YCiHXNleHx9Ux4oVcHCRW0NUxoiXdHSNa0t1BYh/dzUESm9no7pO7PkYTBae6Y42uR/CkuJkpBWrT2bNOs1loCue6wqnR9YgXtxGk/yQNoVx9oB+PJboqWOzSnYaNk5uDJJaW4mrlLo+RWKaLXc9wcnOQ2CJdHSO2N90eowmCU4rruUQqr7j/ZC6rPt1Z7iJNcHy3mDS4nc3h5BVXMRwhWa3EXexMd7qbttNwcXJ1kLjnxKa4ZJm4dSd3B0l89BR37uTqGLGVuz1GEwMn/4WdZ8+6ireGkQN0jRNdpDuaab6syDUlbqNcl9lCKJiY63anu8vsDQsndwep2G0KcJg4uTtI8kcvcrVyV8dIXnl4xj+jJopwTDQKhUKhUCgUCoVCoVAoFAqFQqFQKBQKhUKhUCgUauJq7c6drrtmo1Aoe5wOtT6514Q9AFGosOBUln6viV0al9808SvkomehUCML9vjl0fj1ceUr5PouoGehUMMO9pZ7CTOjkxwsNm3B+abYtUe9uHtQqGEGe4SNWaU39Pq4TfwKuU1+dCcUamQ4Qci3lQZ7Ry9g2wmFQqFQKBQKhUKhUCgUCoVCoVAoFAo1uvqDs3AnoSa2/sOFxginmU5CnFATHadfOgpxQqEQJxQKcUKcUIgT4oRCnCYiTotUIU6oCMXpE+VmfHFatGgliN2sXIQ4oSIQp08++YT+0ZtxxonTJGsR4oSKNJw+0UlvUWOO08qcIvIsJyenJp+c0PKEOKEiBKczd0kVgPQgljwVFvXJOOEE3oQ4oSIZJ+AIcDpz5ozASZjU+LjTypU1gFNNTU17KjmRgzihIhqnM2f0QI25O+VQnNpBDKeViBMqAnGqBZweM5wePEsiWU8nCk6LECdUBOL04MGD6xSnB72EzCU+madxwUkI3QkVoTgJPX1wKTb49MFQbPGZiYETuhMqknEaIsWPH1+LTQ8rTmsP5ac/sptcD9tOqBct2KNtJ8CJyRdmnMouHModRttJzuyhO6EiORUBOGVdAz0OM07ndxa5C/YwUY6KfJyURPml2PSnDwbqToYXp507dza6wWkmnsZFvUg4PeglvjuxpDasifK1Oxsv2M5Ljp2MUC8ITrpORvS8UxRJrw3veae1h/JT7jV53eCEXWBRkY2ToQ+srpdR2HDyn7RrPRkGaCxiIzQW4QANVAS6E/v5pRlN4zEadxGOxkVFsjvpRg7qBz2Ny+D2RfIv4oSKTJwm0lwRv5F/EScU4vS8OGGwh0KcECcU4oQ4oVCIEwqFOCFOKMTpOeWvW9aCOKEQp3DI99Xt1ljECYU4hUPx/m43450QJxTi5MaelrnqUa4/d6t5iDihECfFndKXpaI7oRCnsRDihEKcRhGn3yBOKMQJ3QmF5l4x6wAAIABJREFUOCFOKBTihEIhTogTCnFCnFCoCMbpN4gTCnEaIU6/QXdCIU4Y7KEQJ8QJhUKcUCjEyRInZ+HhQk1wnFwI9xIKhUKhUCgUCoVCTRT9s7N4wT+6EO7OyNB/cxYv+L9diJf8784SK3/HWaLk3zlroqUi/vlnTpJx+rmjEKdIwekXTpJxmuMoGae3nKTg9GsnKTj9vZNknN52FOKEQpxeZJxec/hFnBAnxGlk7vQauhPihDjZ4LTCESdqQh/+/EOqn4fYE+IUkTi9T+UWp9c/eN0NTh99NOlxWkGl3LN0pw9VoTtFPk7vK3LG6fUPuBxw+kgrJ5w+/fWnTL9+xxGnLezHDqdPND/ji9OKFWxPAUcr6F0NUDqcKEWfMTGeXhNRH/9DnCIOJ8BoFZOBJxOcAKY0Jr1BheAEDG0X0vFkitOnsoArW5yAJCoDT0acZIUCNdY4AUurGU+cqw8Ungw4faaIAUV/XkN3ilCcOEzl5RwoW5xeFzAZeQrFabtWKk9mOFGQLlJRoOzdacuWb7/9lgJljdMnWhmIGlucAKK0InJuNcXog7RccgnumLWdPvywdB17OHfpgc80Ud9riFNk4lSSKw5nqY6nUJwoTZ2tseTOidVpH9jgRL2piPTW5OTUbPafsMeJwjTY6iUxXTe08Z4JTlu2bBVP3rDE6ZNPHtwl2WfOwD/fGRWqccHpg9WA09LVzJiscQJzEjgRUqk1KXSnyMRpVbl8eZVue5yoOV0RJVdr7SkEp+3ba4qI/0RNTU0u4LTdHqeLTfxJX6fGn54HJ9/TM2ceeHxPPzHwNOY4VVOcKE+rV1e3laxWor1QnM7NmjWriwSvasI+xCkScYJYrxwOZ0dH2y0S/H6VHU5A0yAhz3p6ugi5lOaIE7nTU9POcfrIEieg6T1CujpvDOaTue32OH27lXTd+JbGe/Y4keIHDyhOZ84oQI0fTiUMp2pwp9WKPZnj1O8NXj9woLRvCqm7JvOEOEUqTh09qcGrWnsy4gTmBLWiuxpU1HvK3p1yKE7kWTvFKccBp22k9wY0nW6kkqGLSrRnhROjyQknUvvgMcPpwbMEkvVUBmqC49RFsq4eKIWvqunEfw1ximSclgJNXaSu1A4nMKf2VP+l6urVqw25CHOcIOrqd8IJwrsbqf4+lorYSnovKvYUitMWxZ2sUxGfMJzukPSnDKcHvdAiJDTqG3t3WqHgtJrGehSn1dY4MaVf/7603+u79n1fbNYBzhPiFJE48cN5qtzWndLSOr2+n8Cc3OE0lEt6XbjTDa+vk+GUQe7Y4cTcianz7+3d6ZqHZFOcHlyKDT59MBRbfGZc3YnKFU6k++r3faTu1Kx+iBMQp0jHiXR3rFpl604cJ5fuNDTo9fe5cCeXOG1xgRN3p6dDsb5rFKchkvX48aXY9PDitPZQ/nBwojyVOOHE2k4t5Nz3t0Ra5jriFNnBXgc9nHY4vS4He9VpPW0uMntD7Y1kbpmzO7kM9pS2k12vCI7T47ukLonhxOvmeOJUXQJAucJpVitpAJxSBk6cOHEKg71IT0W0FZEGW3dSUxG5ZKkbnAZTCRluKsIRpy3OOEGUBxBRnFKugR6PJ05t1RQoV5m9FlJ5gKb3vu9fQM/oYioionGCw7nUru1E7WmQ+J/19LQS30/OifITNe1Njjj9miXKeztvDJY5Jsq3UJyMNJni9KCL4QRx3tMHA3UnxxEnrkscpxUObSffdZrZ89+JJecwsxeZOGlP4/qu2+JE7Umcxl262hYn1iviRE1N+zaO01s27qQ7jftrJ5xCaDLD6cyZxwmEZ/Z8UDdrw5vZc40T7WSkwcm8V8TPlU5GpPf6Z599Vto1hQQpTYhTZOIkdzIivaece0WkdcKx73XVyehETk7OYKxTr4hfi05GL3e1f2rfK+LvGU4OAzQYTp+cOTMUy887RZH02k/CjVPu8uVeR5yoPa1eXVJSwnN7q910gf0Me0VEPk68C2xIH1iTHuWA02pXXWBFH1gAKoxdYLe4GO/0ianC2iti7U5QkQucVtDeRTJLGpoM450+VIH6kI/WwD57kYuTOkDDMELDbLwTHaCxGn6cB2h8ZNKh3Gq8kzJCIwzDBz95e7RxctI//0w/4EkenbHCajTuhybCARqRitMIhg++7jgadzjDB9n4Qe1gJ7vhg+5G437yH2IIoaZD+TgMbl+hkd1cETJDfMzgh+rodsQp8nCyGN1uObj9dfdzRXykH+I+NoPbP5lIU6+sMJkvQoMTo+Y1ddqV13Bw+wuA03CmXvnA5dQrH7HfYc4V8c7knclIhko79wri9MLj9HpYZzJ6x5yoyTPPnsWUYOhOkwSnsE0M9o6VNU0qd3ot1JNeU2ZfQZwQp+HOs/cOTltpIpwrAnEa6bSV70xanF77ucWMyhjsIU7DxemdEKTeiQCcntxeVha+tpO5Sf0Rgz3EKSyTKr8zwXHyLW7pbg1vsCfyeJpbDPYQpxGlIt6JvEmV65alhgkn7Umn14y3OAss4vQ87vRORODkf7LMG/ZURAhL2HZCnEaI0zshJjWRcaq7fft2avhwek1uPmlY+iMGe4jT86Ui9BmJyZHZe00N9P4oZyDUlhMGe4gTXt9puMHea4ZeRmpnI8QJcXKL0zuhDabJiNMf9STpexwhTojTiNzpncl6bVw9SJqW0x8RJ8TpedtO70y+PnuhgZ7aoMKKijgN153eiazTuOFuOxnjPI1lIU6I00hTEe9MwlTEaxqG/vhzfZcj7GSEOA0Hp3cwsyeyEdqIT9sJFnFCnEYwfPCdyToa13pcO7oT4oTnnUbadnrNpCcs4oQ4jRSndyZhKuK1nxtz5YbkHuKEOLnD6R3rSG/STr2izZJjrwjECYM9wMlZAicXwooaITg5S+DkQgInZ8k4OUvGyVkCJxfCo45CoVAoFAqFQqFQKBTqhRNm9iahXGf2/qcL8ZLuM3v/w1mi5L86ixf8pQuNEU7hmQUWT+NGFE4vOUnG6XVHyTj9ykkKTo55cgUnxzy5jNM/OApxQiFOiBMKcUKcECfEKWw4vfUW/5u8OK2Qfx1x+lD3D3FCnPQ4vfUr+bq4v3rLCaffC71gOLELTa+gP9rr4s4xvXJ7yCWmEadIxmkJ6KUl9A67tcYp7fW0NPhzwoleFFe9bLstThQkdtl2PVAmOG35uy1Uf8d/7HD6kv2OK07ai7Z/8IECkok7UYg+Yyh99lkIUIhT5OG0hOsl+Z81TmmKXtdCZcQJaNquiDqULU6fytLyFIqToEkhyg4nqnHHabUsRpTWo7Q4UYo04hb1IeIUsThRhkpKlqiyxCnNIEt3ojTl5NTU5ORQnlR/CsGJW9NFKsqTLU6gb7/dosoSpy+FxhOnDz5IyyXd5SWrq3P9P60WJiUTpcepdB0hDQcOHOgjJHhdACWbFOIUaThRmIpI8HsKVEkuuWSNEwDUCYd+7rO2tLQcKGmJEzWnIvbUnT4A6qNf2eAEMA22EjK966LOnow4UX7eK/KSu7eAqG+3kj5rnL788sxdkn6G8sR/xgGnFR8AR8R/qboacLqkutSKUJw+ozilXD3wPewF33WNSSFOkYlTSU8qIefAoFZVM5yWWOI0yJ/qbUujJRV7MuBEaarhOBH/CWpPtji9x5+7U6O1JxOcNvFn7n77rRNOj+Fx1ZeqxgsnUtfBcCpRw74VBpw+5Dj5rn0/q4zidOCAAhTiFIE4UU+6ReiRLykpoZCsssIpLa0mnzzr6bnlJQPwrdtT4oDTs/b2wVygBFpP1jiBOW0mXe03Br2kzwYn6k2EdN240URInz1OgM8QPC4+MwFwIkvbetYBTiXVXV7i6y5fzbMSepw6yshdcm5Wv3evF3Aq7UrwL+0jDZwnxCnicCppyyXPUn2XyjlOJdbuVJPvpyDd6jpR7cKdAKf2WyRY7YTTNv/QDeCkq08b7YXgBAhRX/p2w7pbAqctVjg9gNpJfE+BpwdJ6QNJEPeNOU4fMJzukuApilN1dRHx3QW4SlYzezLi5O+KbZh1i3S3+K5/3wXRdGwS4PQZ4hSZOHV6008VkaXl5eVtdjhB06kRAr2hnmoqG5x+9dH2HI5Tpxt32gAB3K1OloywwymV2pKQDU5gRpdIyuO7JPvMmTMPkuCVlC/HC6ehdaSb4dTT9dWptlukrtwCpwFv+qVWMtDiu9TvJee+P1VGGg4gThGIE9BUfoV0d9yKTZ/lgBPw1L6OtXJOyDilmeH0lsDJVdsJcLpRxJMWwJM9Tp2UpC2OOJ3pJdkPhkgKxwmoGjecBm55fUOAU1t1W1tPX6sNTut8Ay3BEy2+a32x6Ve/B4uiOH2IOEUgTj1wONt6ysiAsztVV3d2tQAjA9Xtzu5ENdcps8ey5INXoBnu77uoaTzpcaI5ci/DaYuDO31JIzzf0wePk8hThtPTM2FuO1XuPOot3nko1UXbaaCniNxpAZzabrXQV8xxKl3nv9ZFer0pP1GcSArgdAtxilicOmP5M1kdju5UTQO9znWkrq3d3p1E24mdeLI578Ty5DeYoOJZ46QJ9m7ccHKnIfHWtRQn31M1FxEunA6VnXSJU1snFAOcOsGlTnXG1olcRChOfXAMKgGnS+BO19GdIhUnftKJy/eTkzsNkmAHTUUoONmnImpqcpx6RQBON4ivE3B6T58pt0xFbCVd9u505q54a/pTGafwutOhs0Xnz7rC6VJ12xWKE9tjlm0nihM0mcg1wOn6Kdp26m9BnCLVnXpSfRCNtPWsI0sZTqtsMnuppLe/p7OMdNu1nVScqDVpaTI973Qxn/R23hiEW1t3EonyDYTGfNaJcoj1aFIPjOllUgs4BdVYL2w4PWq6l+iIE+0Vcam6uief4tTpJd1dXpIeitPPOU4d60jweofI7BGShDhFqjvdIikd5SD48uxoc3caN/iTQ6Kc9Yp4xmiy71GuOY3r67TJ7FGeMvgzXd/a4zREis9QdcH/0cHpws5DPzrgxDsZXVpdUjIYS887QdvpzlCZ76cPQnH6EHC6fqCLpBygOB3o6PL6lnZhZi9C3Wl1Llm6qgTU6YWvUdtORsBTZ2ssmd17Ko33irDvZPRsuyZFboPTpzdavWR2V+dFu14RzJ+KiHMnI4j1atm520vgUgynfwg3Tg07j1Y64UR7lK/WiXWNCOkVYewD2/HsGWs7ncPzTpEZ7KkqKVll2wU27XWXXWA/+tVHojP5r3TmZNKjXN8F1h4nfRdY8x7lX/7Dl0aFHacn95occdKM0FhNf3Sd9kIGaKhEla4j/jtTaOc97BURgTjpgdLSZOZO+hEaNuOdoMlEm02Og9t/736Axt9pO5PbjHeSO76Gdisf6+GDK+jgQZ1WmI7G1YweBHvqSiCk9xo3J8Qp0nBa8hIf4CSGOzmNxqVEOY/G5YNx3zJ403MOH+RDntT7E3w07hzNANw5P1vxM4vxTjppfAq7wEamO41gcHua81wRb/0qhCWnwe2/dzW4fYuOJXucvpwoU6+s0A3GtZl6RQ785AFPiNMkwMmFO5nBZDn1yu/Zzws1V8Scnxk8Sr4/x2EmI/2cEYgT4qSFyjnYe2FnMpqjAmSAy2FiMBzcjjgRnGdPxWmOyeR6c3CePcTJBqd/Ch9Ov3/x3GmOHqI51hODIU6IUxjd6fdmRL0Qs8CasjQHcUKcMNjTqO72sjJXbSdjwhyDPcRpDHCKrGDPfye5O9dlZu9nZmwhTojTaLtTBE2q7P9qWYvLYG9OCFsY7CFOGOxpYJrbEnQI9uaYXzljDgZ7iNPo4/T7yGo77V12uzXWZWYv9NwT4oQ4oTuNILM3x7QJhcEe4oQ4jSRRbtLRCN0JcUKchotTqDHNwbYT4oQ4PY87KVDN0WOFOCFOiNMIg705eBoXcUKcngunOdaZ8jmIE+KEOA3TneboT+POwVQE4oQ4hSGzF+JPiBPihDgNL7MXMgYXM3uIE+IULneag332ECfEaYQ4zdE0mebgaVzECXEKd9sJgz3ECXEaLk7OEji5EFbUCMHJWQInFxI4OUvGyVkyTs4SOLkQHnUUCoVCoVAoFAqFmihynYr4NxfiJf/dWcNtErvfzP9yIV7yD84io1byD+EsKVb+t86KrFTEn53FC77tQmOE0984ScbpVUfJOL3mJAWnXzhJwelnTpJx+o2jZJzecJICSfhL/mGmo/4w3JX/7f/npL8d7n4fRqL8LScpOP3eSQpOjok9Gad/cVRE4/Sm7Q/iNDycZtr/IE4vOk62ehNxGhZODjShO00Wd3qT0fPmaxPZnbQVk/7aQQIvL4KfN4wFTUuGlnq+YG/mTPl2orvTG4gT1QpFDjjNmzHj1RlO7sQpYki96exO777/7vtUv3gf7tvjtOJnKzT/ngsnyodG9p6z6A2rglYlndzpDXqzSPdjHewp69bTZNJ2+pOQK5zeDzdOH7Freb7xlvH3OXHaEmE4rdDJGqd5suxxojYkCipsWbsTgLRE/IDetcNJt5m2OKWxH1t3WqTXG4vsIAGtBLkAb5Gm7tu6ExBkkIKUzp14Mb5u3UJN3AlA+pgqFKgQnN6X5YwTu9T062m2OL0BPx8JuXAn+SLTTjht+VdxlWlXOH3JfscbJ3qtafUq09Y4zQA+FoLg3wwbnACaebwk3PKo7zX5nxGnd8Gb3l+ySogRZY2T7nrYoZfw/S8tTEwhRGlwEoDIMnCih4SVzcnJCS0XWtJigSbBnn4D6BtM3WmRYZkzhbuZZPYYTJ9//rkJUEacYEezPR7KUwhO6lXb7d3po4+2UzGegC0bnD7VXLXdFqctf1au2m70qBCcvlQ1rjhRmFbL0vGkx0nApAI179V55u6kK/imEv6ZJsrZYS0HMaA0PIXgRGliWyhvpzVOsow8aXFigCgS3/6LrCAxFFuktI50JRcpS1UKqo5idKeVMqIqLaHuNHOR6TIX8eaeHidK0+dcjCctUgacOEwyUO9r4z4DTmka2eJEaYKN5EDpfcqAE2B0kSmUJyNOW7Z8yxQKlAEnAdInHKcvxxentCJyrqSkpNNLesttcFq4sL81ltwZYJjowj4NTtScoOBdQu4sPaAUlJtRRpzefX9Jo7xBA+W55LodTmm5pLsEWKrOJwPAkxVOaWk5nXQ7T4QwpeIElbQml5DempqaQUJ8/TlyLLfIFJKcIv44WK0BKqQkq/mDdNV9+rpvghNfaHd1Tk5Nrv9ETs1mckLh6Q9GQpVlGoAy4tTh5Y99jz8XMd+fTHGiNPW3eomv95QAKuRrTINTJyvZL5BKM8eJ0dRIfD05Op7eMMXp4mArIdO7akJcKgSnrexhUtcNo0cZcTpzl1SdOXPmUixZa0BqrHH6YHV1EVnaVtKZSurKLd0JaCrt4k8s/WyhEs3NCMGJmlMff5zFeFoogHrT1J0MOC2Rj6sJTqtvkfQOin1s8PvVljgBTVf4M93VBqA0OK1kOAV7amoaKU41wihE5TfiVKPBSR/L6XCCmi+vOickjjTgtJIu1H8CeFZwWhmCE4sIzZe5yB4nFvKpQZ8OJ0rTLXmnqy5lhhPsPaWk0aWMOOXcSCXkGTOo7WrcF4IT0PQef3wnhCc9TuBNW8UTd78VQd+ft5jh9CXFqZbRVHzGEPKNA065gFNPGdnbsdoOJ4Bk6axTwNS1hWo0F+pO8+aVl0HBjj6vWlCO+kLd6f1V5W3Ax6mOjvLytg56XM1xAhNd3e71Xyopqb5CskrscAK/edbTA5XwhBL1heKUQ3Hyn2hv38ZwqqlRAqoQnKBsEXnW3t4uCqnldCWp4bBVt9NV5xiLGnGiCyV3emracylUsHATnEKXqW1qhQZ7Bw5cvXrCSxoOfK5GfaY4dcaS7lMd/etI8Hs17DPFaTCW9Pb3dELJDgNPWpyYOQ1SRNopT+yDKzwZ3eniZtLVfmPQS4YuXtSHfSY4dd24ceM94u9Ugz5TnB5QnB4nkKwzIuJTgBofnHrWkfRTJZY4zZi3sHwdWVoKau0FStq6IAJg0VwoTgvLU/3XOjo6urovLVxY2neXFqQ4vWnRdirv9AZnQfOpbR25tMrOnWA7u9uqaay32hKntDTgpLu6urqmsfdEWk1+sK9s7k8WON0FSAa9c72+E+25vr7WWN+zHDucGHM1t1rInf4cM5zAcDaTbigFq+6H+gQhp7+3J8cOJ7pYilN7LsBihpN+mTXbKFNNpJu1tEJx+vzAgZ9aSMrVA9+XBS+1xgbPff4xtyc9TqsgDujuoHv82YmOcn4oS8We1+GUlgaBC93l1e23++Ef/ewnZJ4MONHPM5QKnwU++Q2ITuc+y9luhhO40zb/EEDS1NUHJB0pI3f7LtrjdCOf4rTNfyt/dqcNTo/vkhQI+L58kJQ+kJR+ZlxwWiGqaSvxnai2xgnMqcfrvw40Mbcph+LQPKoMxYk2nUohNO4dmEXZK4VYYXYsafiMR3smmb0l7nEqodFeGy292sad2uGYQgVg36M1+TREKzfHyd/l7e25RXrLKE6wxbDVQ7zym+DU3c7sqQZcwgOuZoBELJOuWrGwQXY1IF+/HlENTpTnYL8dTosMy6Q41dQ00bjPAqfvW0nw+gHACT5PL8QRn38cghN8g/WkkkvlQm38UC41x6k9lQxUyxKf3QwncKQb3mB/I0U/pz2f3IUG17OVnKcQnDbAxt3qvEF9qYktsk/YkwVOm8jLNwAneGH2DWuczsHefAo4nXmQBK+kfDmeOLE2UZsDTsHrgiYwp69mddxijaMZocHeQgADVHeptLSthQyU9qQGr/Kkudl5p1WrAJDvy8tXMZyW2OBEo72BNoj1yjU0hbhTu9f3k6CpGg4sOJVFsOcfSqUVYCif4dTb3t7I66kpTlRQr2+kQuHB2DvVpjjd8NK4UVT9fIpgEemttsZpCL7HOnNpyMlxWmSCk26ZKk4rF4W0nT4GnGgofoDhVHn1aiupFPZkwKnT6wOcWKvoXI84lGBPJjh1sp3JSi6F+yeqB2PrykNwYuZ0BXbhYCxtjsL+6Wkf7OrPscDpBtudd/puXLyR6u+DsI+2okJwomk90XZKorHeNmhBfWsT7FHVCpyywaTGFSf4hgr+ZItTpwan0tKOU0OtJEVEe3p3Ansq7e+aAtXvWmlnbPpVZmkWOL37CxmnVRynVdY4sZxJd08uGSixw4nXgGoZp4HqNEucivzAUh/Haai9vckZp0Fyp7O9M9XXw+qzDU41tGa1QywpFzUL9oYGvf4h9zjVOOD0+ef9XlJ54MDnFKdrV692ucEJovL+PjiUItqzwekWRLk9nam0EWWCU3u+H3ZhPhmqge8c4lvc11NjhdPFi4NXwD4pSWRuJ8Ryvk5Td/pWTUUwd+qzxwmqcPpTjtNThaYw4bR2ZxGpPOp1i5NvoKeMdJfTIMom2LtGyeifBbj0TVFSdyY4dcwq7aAN3eLv+0jK93Y4/ULGaZUTTnK01+cN/rTa1p1YsAco9UDIn09jE0uc4AvVe6dTj9PKRRZtJ9ZyGuQv+PvNcWKBGUQ79Cua7AWc2lNZtGeFE7jX3DJ7nNqVZXKc2tuvmOJEYz1oOGVdNeD08Z9Mg70BmvmBBvO5jj52AeU6c5xEsNcDJZeKHJ/vp1CcaCJCXOmyDnbUYCrdR0OW7sRURO60vyfvTttgbzAf/jGclP4RJjj5nj5mtgQ4+UYBp6OpbnBSMnttt4iffe1b4SRSEVDpz5XCl9bAqb5YE5xosNdJ0q/Clx5EEN9zd+o/dcAKJ9p4EjhBA9km2GM4wdG9S6n/wLqTkZKKgA/lgNMJWgW62zlOZl/7Wpy4Q8DXaV9fX2enabBHk+8sbZALxV25Exgdzy+a42Rcpi1OH3/+/TqSDg0nHuxBzGeOE09FZHWUd3TAV+g5OJTP4FBa4ATxQB1NRfTkU5z29vX19/e3meFUI5/wYGnS9s4r60iwxwyn3396g/g6Wb6O4jT31iCoxhanGxnUnpxwqn1wZgiY4jh9GXacdjYODyeIotJ1mXJjohx4WzrrFLRcr5f2ASmi7TQv9LxTWyrpPjWrv4U00LbTudL+VP91a3d6X4eTZSqC5/Zo1KWP9ULcKW2Q+FlmGSL9mnz6Xfob8/NOUI2hMg8ZcDIJ9lYynFi8BW2n/vbBBV1mOLGkNl81zS7Ibaca87YTXSiUamIxpGVmT79MnmHMt8KpC8Lrq1cFTo8FTn/6k12inJyDo0i/+UxxUhLlfet426m/unPBs5C2E02TU2Om2Rr2TVIGDVHYUz0W7pRPejup5fTegEJwb11XjZM73aXBXucWW5wApCiSRXEKngn3eae1hy4cuuAWJ9ErIpYstcNJPo17rhTaUaS7y8vaTjOsT+PSthaPEBo+s3YnBacSZ5wg2iPBjtV27vQb5TTu0uo0S5wWcZwgyu0HnPo5ToPmOLEODM/YOZ8cWLb/bqxczoiTcsqVwmef2WMLpSec8hknLk7jwhbkAHwvexNMM3t/+vjAOvnYnqM4fW6Dk3Iat+4ncSjTzVIR2tO4d05V88++dLUZToMkvZqaaBPZWw1tp7mtLbCV5u70qQjxfJ0XL26ARcIGXLTESUSDnQInh14RA7FA1ejgtODeTlc4KZ2MgCrfT1Y4sU5G9Euqd4DmIiDgvjPQ4rtqct6J8kR7I83tvkqTFn3L7c47saPb6U0XONl0MuLJCPCTbr05hZ7Gha9U2E52goThZN7JKIcmqOnBhzL9NdQdcixx2k5xoqdOV7LzTrOf1Zicd+J9+9iq+3im3Oa800yOE8unO3QyEsvsZ8mIK7Gznw064wR3H3/++S1S+XFoolzuZJRAZvcOlJaX00M5VOa7apIoF52MpkBJeu6Bnnea+6wkzSyzVwQbxezbCx+nvdVLd9J2C5w+vUFf7+pkmfIyuGd+3knpZETu0szeZmucWK+Iqi/ZvyDH6V/CjVNqpVuc1C6wtG+mLLRtAAAgAElEQVSpRZ+9GWrP1oWaXhHzzLrAzjMpZzVXBB3ttGQJG6dh0ndMP95JbOkHdjhpusDq+0QYepTr+8AqHQ5CT+PK/cTFSAnLXhH6LrArtT1XzXBapCkjejg5dYFdqeuKOzM0FaHVxx+Lbka2XWBVvW+K05w0E71ugpMidYduNz2Nq+0De/FTfV9YPU5/VrrAfvutcaCGsUf5l0aFH6f0R25w0g/QsO5R/uo8dYCGDMy80E5G+gEa85z67PExGhq9K8YQmo7GlTfUafggP+or036j71NuPUDD0MEuZICGPChKfpdpnz3dAI2Vi2z77M2cuchyhIbWnWaGbmiO3MfIqkf5x6pM++zx0U4KRfpOezqc5hj6lOs6lutwYkB9tF2D1XarTkZ8hMbFT7WyGu9E9a3ZII3QARr/8uUvTcdojN/wwQ/shw+q4wfnGbqUWw0fnPeaOpDwTcuZjN59/136+y69VQbkmg9up+Trxg5ajcZd6Ti4nZsN+wkZl2scsq6+YhyWqyvJBs5qFieWbTN8UDuG0HQ0rn74oBjHaN6jXBk9+LE8PkPtUv63ZsM2DbIaPjiHjh98Pe31D16H3zTzARof6cXA+si8C6wA6vccok/ZXavhg3+mI57+zHq+/vlf/+xqNO4vAauJM7h9hcNcETNmqPdmmM4VoRnc/qY8ctB6vBMb0P6uPKz9XeXGcq4Iw8h2C5yMvmQ69YpxOKw624MBp5naeSCUojNN54pYZETPdq6IRTPVoe2LzOaK0A5u1w3dNZsYTGXIOBx3xIPb54g/fqN5MnS800dvGcEKx1wRtA/5n0PHuL8AU6+8Cfy8SUFiv+yu+WhcZfStkMyU5UxG76o4vTtGU6+YTI4CFVc8bfAcioY8QYsOLSNOM9/Qz8BiP/XKopnm93UzGWmmXmEzTMh33xirmYzm6AcNzlGeCJ165Q2cySjsMxkJI3ozZNoVq2DvXT1S4zKT0Uw9CRbupM7SYDmTkcqckb+Rz7OnX6XyzASayegNBaU33npLM+kK4vS88+wps6yETApm7U4aU3p3/ObZm6mSYzHdl5uJwYY7z94bYlojS3fSzF02bvPszdH8Ws9k9EaIRYVlJqPJ7k5m5mSXiviFmT2N37SVM50gmRn2aSvfsHEno4eO+Tx7IdEeTls5Hu5kNqvymE9b+U/DxGmmEyQzx3gWWGuaJtIc5SK2e8M02kOcRsGdcMr/4bedcMr/CYRTfHBZ7mR3p9/8pjoRNZl0/swo4RRcdrts0rtTdeKy5dGyeMloj5NEwdEoGe1CrkuKlU9zligZ4yyxcueCw96bU50lSk5xFi84N0R3liWeGRWcgsueLPNOendKXBZaTxGnFxenuXOXnR8NnPzdt2/fzp/07pQYN+Fw8jj9aHCyLzkinKZZ/oTgFB0THW11M2FxupM4OsGevzuXoDtFTzCcPJQR+z+lpChreRtmd5qmw4lDY3ozoXGam4iZvcmDE2fEY/c/XnEnj+xP6o32fvzwcZrm2p0sUFIpG1ec4icFTuhOLt3J7j8v6dEamcl9zyi40zQVJxuaxM2o4RSP7oTu5L7tlAyPPHGUCPlGfqx3Jw8vKp6O0ziTuD9e7jQBgj10J3Qn4Tkej5xkUG6ixf041XSEG6nIeTR3KWij6052badRDvbQndCdhpPZEyajBG9xHuW/ajqyEykAyvfVjN+oupPIOZi3naJj0J3QnSaGO3HHiZZjPE6LxrY07qRpUqkEeuRm1Fi4k9VZJ3QndKeJct5JcMTdKFo4k8xKtM6duHd51DSfYmdjkdmL8dBfww380rNP6E7oTqICNJzOlAJH18G95AtwN+9oy1i6kzZuU07Kqv4jl9R4l74VJexs9DN7NuY0EdwpHt1pQuDUUJB3KPG0dLjM46ks3HjsXoW0ewzdKc6jNRs58lONKF45jav1Lo+uGTUWmb1oYUaKJyn/0J3QndQKELcn0OjxxK2XNoE7tVKzKtiXP2bnnTyaE7c89FOy5FrTidb2MvLoTk/RJ5JH3Z1kc/IoBTzK/zFzp7pHBVLgZi69+2OFJG1sRHeacO5UV7GvjEJUuF/EeHvXHMwdwy6wmlNOHjnyCz3v5NEGeLr8nxwsjnpmz6NgZLw3Vuedjtd/c/tR5uGyKVMgjLh9vuLg1knlTupUESbmNFFwyiqgYR5QdVjgVLdjrNzJo+0uxH1JIUpGhWg6GXl0nV7j1Puj0aN8mjHYE9kHQZJHm9cbw0R58p68oilxezaCRzUU7mqZmJk9ZwmcXEjg5CwZJ2cNdzP/y1xmOEXXrckrgocUJ/5CZeGuqSYjH9yPkRjOsAtPtKZvq3oSSoVM4076Tq8eXa/YEbmT2wEaLhQ/zH00cpzW522eklVAQVq+Zl++I05v60RQ4VOi6bO1EIQv+PG+9DUfEOZbH6CTy6evkTYpBQ6nuhxW9kNgl3c4Y6Qd5brkqO648Kzdd+H0fu/zrJ3t4jVwMNYWbmJH6uA2h620OOSo0cPJd7xQkqTLmbv5w+ICdsxHhFNKgXQwH/czremSrN3yc5UVUuAm25HFhfylTWa78P5GeWdn/VAoBR6yS/DMj4uL4yQykrIzM+j9qrzN6nfiYa/7Q44aPZzgG++rZetqAxn8/h5+jEaEk+/45SbczVTHL3MVBOTLMh3PDBwV8ysUFwaa6YsZoe+rLJBknBoKpLzLzVLgCPuaElwG9+xLRZwmNk6MHmErVYKiEeGEMtJRKEJouJe3QX62uNC87pPgIymvUOCUskPa7YUvKOngZuL7atmyZeyKVccDG2SL0gV7iNOEwum4CErWForwHnEKg4JrAoKhlB0B1YuscMraId1cViBwEns9uEYNF+nh2e1lQTU9StypJiBO/9dZrvN1/+46BzjszN7/dBYv+N/NlWg1p0ny8cx96+idhoKNufypOsBJFOQHNqtg/5PTkrQrOvrHe82ZklR/hOb/4Nnl5yskKXAI3k+bDLu8JDo7ky+loZAmDWmRRxCt1DdG/0i7M91cFx1hU6+MeDMrC/eV8XtV0v6pSkHAqUWk7/aukQ6Xwf+GgrzGqXX3j7Q0FG7Mpy8k7xFfZ7D3y+S0XkPBfnY/bs/BIpYoV07jQqk408zef+g0Rjg5nneScXrTUTJObk9Qkf/2OycpOP2Tk2SczKd2TDTrmODx1AEP+9iZ26wdeYeOgXLpyVzaTYIVlHGqpxF8BiAnSc0UqN0Mp4M7pAB99HWLJU4HT0MRSTp4L1NqLuQl5RM6YZ8iaFg4TXP4c4lT3WnRUrr8sEi7TXF7xD6EvZm3Vd1MDU7AkbSJUbVbPBY47ZWNbW3hxlxBU9aOjbdBucpp3CJnnH6pFeI0UpzeMvmxwKmy8Lsmdgp3732ecQpsMMVJOtgYfaclOvn8FfiijVsv7cunrEjQwqaPgBwrnKRA09RoaGQDtNHJVazkhMBpWvS0GDuglLNJNtMY0d/iAjmNR/trqQI0cuV7+y6Ah9fzZATL7NUf5Ugdl/K2wk5hHqXBqa5CJDGyCvI2c2rgkDBlwH2aJnxYNMUNTm8rP4jTSHF6axjuZCoTnAIZ2q/khsKDuYyVXTzoA9+yxIn6GEQveVtZycAGFSd1ai3tP+VmlN0p7MGebpOS1yudiWulgJR3GYBi7aEscDMg6vA6yg1Y2OEfCw8WTdXjRCmScSpy7lE+Ad3pt7+FX7hht/T/JHEn1zhtNcOJP0uLW+LEi1RJrCHBGmUanHQjx59/EoZh4DTNESe1r0NMsnCiaIZ5HHuULJ6wwAmiXDn2A0umAQCN7HjJqckXCkR8l1URKAxkTB01nFR3ensMcQKW1Mt4CqxscZr35rxXX3WD05sz5KsUzrDH6aXfLfndEtBLYWo76a7R6uhOohOPC5zu/Hhs587TkhYn+I7d7YgT68a0V4tTtHa+hRhXkzBotjEM7jRd/tX+iWemKe4kqImJFr6pUYx126lK2tVi8Kkque8Ji/JEgHc8E5qTRpxMgr1Icqff/o3mou0yVCpQoTjJV5B+81UnnObNUK5GPcMWpyWKfveSDU5p8MN/0/7pdWt3ogwtWrRI3MJ/W5zUCqLgtNscp70/ZPIYXotTsjNOtSY4OfJksZlucHqZKUzuJLMTowAVE61gZt52qtsh0g+Ak5yTyM4UuW0OTi7L4VXRXWnEae8akVlvUFMRkeROlKbVQgpUSsgXghOwsRDEibLDacarJpd3t8Zp1apVS4wOpccJKAL9Uxr/T++au9NHi7YzreT/gCcbnHTfuAacqtg5DQWc9VLgUOvy6MrCjdY4HXSJkzyjSbR2HhNtCGi5mU44vaxI89i67TQ9RmNQSp9yXdtJw5LRokypr6UpTLGlVWJnanFaW7iPgQM78r60v8WAE92hIYnyEeD09tvj4U6//e0KgKmES4FKNSgjThwmGSga9L1qgdO8ebqyMyxxYjCVlJSXl6wSBvWSGU5poTLF6aOPtm/PUQVA2eDE60RUlFpZodZ/zUKVaN8eab8Gp7oKaVMUaK01TpWFHKe1Lt0pOiaKSWkwCbxC3EnPvA4sA04vv6zjSYeWxp3ksC46RvUqNdrTuZOyZdrEidKeCt1MmulWthUwKuNB334l2KviIV7djkBGQ0Egw6PHCWLBjbSfCuz93VPc4PR1sk2PcmFPY4cTmFMan8bc13uqpKQ63/cTB4rzZMCJEtK/jpA7Sw8sVKI+i2Bv3qpWknIAYOr0kmsae9LjBOgsaRcntn3XV4mYzwynnCLSXZ2WVpPr/ymtBjZTC5QWp0Xba+AD9dbU1AzCIvtzVm5P1HytGyuAck49SVSB9RKPVWhmbhNRcIpKKWAnROJr4XBb4NRQCE9GxUJNgOZ0PC0SS2ab48QJimUP42dHMYyiYxKI33QgEV1TEiFRBmsIxYmikwQw+GcrUCURvwEnkYoHjmDzNCZlmtlj1CTAIuOTotRQzzwVwQpmZx4ug02LPXn5yJTouh3SfuDpZKHchW9q8oXCvEagZj4jrFY6WOTR40Tfkkp8x8HpdezEkqRQnGBX75Jxmk3IbPgXT/wUp08++QRAenus205gTtXyVQHSOyhOl6hNyTyF4nRLdAw5YIj5QnGa1+Ml50pLO9aRhs8scaLupOB0iRuUGU5pabCZ/hPV1dW5cNsOOFVreNLitJ3hFOypqWlkOOXkJGq+zh1xaiiQDl6h2agdEusaJuOUDraVyvtqrrPACWrC12VRe3+QKE4kxQ4nhkxUrFj37ChuVRSn6NA5TViNjlU3UctTCE5J/LFfg9N0zpOh7TSNrn+2m7ZTAn9jfFS0AlOMCU6sYHBPIAMKemB3UauG3RWgiXLaRyh9TT1NlAeOUGqgnZlPS8MeA9wu0z6v9Ze/K2JBIMutBzZMccApeX09LaY4EgNJQEVxAqDeHmN3Ejgt7enpueUlA209DCfBkxGnVwGn8jKydFZHHxiOEshZ4gToBa+X9sUGry+0dacl5eVtbeBh3R3lsO5VSgsqBCeyt626XeAEZKkRnw6nHIqT/0R7+zaKU02NjFO0abBHKzFJiFIDvpNiGIGU10gUnKKiYmszpXo4zBsrDuZGRZniFA2Na9pTYv/6wNakWIFTlAVOMQynJFh9LPHzoI/iFBUdOmqcbiWt0v4oB5w4TUmzZ8PtbEuclEG3WpymaaM9/XknsZmwSH1rKgQnDxSEllEqLe6rkm7S8wNstMV3V2jBlNOZsH9uFvF8eGAD3e9ZFbRzRJWc0dhKhw+yGaYeGrPkoTgt3yNJ9U1eBScgyUf/5io4UaDGw52WtrW19ayDfz1l/qFWMnegBHii+QijOy0sT/Vf6+jo6Oq+VNpWFhxqCV6f96pV22lhWxlp6Cgj5xYutHWnJdBwgrWnzyqvpouce3UJw8wEJ/KsR+DENvOEbE8qThDrUZzukmftg965XorTYKL4ZjVvO9H6nMAqMzUAKJd1r5mevT+UT3Q4+U6y8/up6/OKYtmzJN6IU9xxWuRIS3ZmRoLAKSnJMtiL4fU0KonhlETLcpwM7iRXacomC/tiSXyC/ImMOMVyX4qPny3YMsFJ7hNBcaJ/YEZJvCEV6k4xbN2z6QYmwS3sKrpQJScRghMtCHEh3974JENQoI7GhRCP7vcE+M8+j8fjMJORabBHpTaY6JaJx4lJJOupwGlM204yTj19zJ3K4EsIvjYGaPvJDKfSVmiXDJzqKC0FnGiAeEDYk5k7LeyL9d0lKVcBJ5vMHsWprRVCPTAptsjSJRbB3l0S7O/hOMFmwu4cEPZkxMnf5e3tuUV6y3wn2gdjWffi2bpvc03KjGLErUGOaPQzQIhsBf+KTmBVi90kiejHMLhdMCIXhCWqX+t6d4rRulMSKwj3Quc0EbEe/MZHMfrU0CsEJ7ppmmYTX+bLOpyi5c5EMk6EjnedHRM9zaJXBNu2JO6fcmm5VaXHiRVUvpoIj08t5orwCJw8fCuTwoDTbNZiYGAlkrnE93TM3em32rZTbxvFqbut7QqpKwd7Cmk7UULa2PiTuksMp4bS0oUW7gQ8LWTwkWulC+0S5cydoEU2UA4eBasvL19lhdNQPumWcertqYbNrLbAaSg12N8I5QGnfJJIq4HgxCQDLXCidZvetcRJrsaOOGkLxrMbE5yiWXWW204JYu0cpxB3oitLAN55RWUlzXFKUKM8ihbEffFGnPTBXhSDOZ7lQKbFmGT26NrjRcZEfKCkkA8kt53YB4rn3xHxCcx37XHyeOjngY8Wn+B5bpyoPflnM64Snz4Yii0+I3gaD5yCA20MpwHajgl2mOH0JiWktL8LPoj/GsUJSFk4z/I0LnhZjxeQgzIzXrVsOy1ZsqqcNpzKOU4DQJMVTgODXv/QOo7TiZ5quplWOBX5gaU+wGkwNpgYpXJicqaE4ySgMuYsjDglRbnEKUlGlFcqA05ysKdUP8IXaYKTbHkJCXIbJkFZuS1O0BKbTZtRJu7EjUgO9tiKLc87seYlTRdyuzX9QKrTs4JJUQmy8UbpE5AmONEvCnb3OXGaPnc6Ne7ZDKvEx4+vxaaHGaeGezsPFbkL9m55eQOqzHcJcEr1zTJ3p3kLO2aVdnT0ryPF37eV+a/bpCJenQHwla8j5/TmZOJOJUBRXQfFqbrMz7J7Vjj1FJE7qSIVATil0nS5OU5XSK/3TifFiezlOM12wIk44ZREy7jBKaRgKE6yOyVpkhD81hSnBNXxEpjtJTgEe7NnW+Kkdh034jTNIrPHtzCeO+1sG5yiEvj3UryIdd3hxBUGd2LBnp/jxOK+8OJUvPObxRd2FrlLRVwh/gFnd5rXSdKvdnR03CJ1jjhRe6I4LbTFCcwJNiB4qk3ByTpRPgAE0aQddaeBaupObSE4scyeH0yJkO72YbtTQoJt2ymJY+LcdtIXNHEnte0UFRWjdadoM5zkqJCGhbbuJKciYMkqTqGZPUt3mm7iTuKLhmVMbHESKdIkjpODO02lYV7C1KncnRISnh+n6RCyJjF7ApyugR6HF6eTh1JJ+qOmWGeczrHEXnpHW08++IRl2wlwaksl3adm9bdADNdW5ru+0Po0rhanGXY4lXCS2xhO7FSuKU45FCdoLwmc6szbTvy8k/9EO3A3BDj127edPCFtp9mmOMkZhlhWtbTNF4tUhFxQ1FUznERRlj+LEpkLc5wSYtXY0b7tJBLlNFvAnIq1naY7uFOMvTtFsXYQz5hYfCAls8cDt3gXbScFJ5qQSIhPSnjuVARFabo4+QRtp4G6k2HFyX/hqJf4Hh1xg1NJSQm0X5aWV+cTrx923CWzzB4977SwT0wHcN0ZpxkCJ5056XGiTacS5eLy5yhONr0iLlVTkDhObDNPmJx3WsRxyiUUJV9/jcjsRUXb4aQEVBaZPU3CLkmfXLPK7DF7km3MBifRWS+Jp8z8MaY4cX9g3/t2mT3Nadwkkdmjy3Ryp5gY+7ZTgmKNVh9IPY3LAzdaMFacHHfAaao3TJk9fsqJ3U6PT/TdiSW1Yc3s+V24k+hkdI7227tCgj9V5wf7W2MtzztRw4HXydzuq9Augro/b96rdu40bxXgNM8Gp98ZcMqnOP3OEicI+QZj/Zeqa/hmnkgzxSkHcKppInuhmMN5JzkfFaV0PIgydoaT65QwiCQRlZGkBCW/FYKT6BTE6iq9F5rZ48zQl+UZivnZJH+MWduJYce3cLZ8hsoKJ9bJKJ7nI8S5LKe2k4yTVduJdTJiK7T6QJpORlAwgXYyoieobM47TWW+FAUvTU3S0TRinHjvIuZRc6cnRpH02jCfd3LRdqJdYJUO5VRyX1izXhG6LrBy31a74YMzQrqTm6YieAdY2iGCdyu36FFuKpMusIu2r8zRybpXhLFPuUnfUsOLURqNeFJlZQh7tOZuDOsMG22aitCuPymJtZ2SzHDSdYF92dC73NVo3Okm7uR2NK5pCac5yilQU9WTuMO5IE1IolzTBfYTpZdR2NpOfprZa4x1GqChjnfSjNQw7bP3qjJAQ9MB9lVrnMSIpxkOOLHhGWKAxhLRI8J8vJNVn3LdAA0+QmOlPEJj+3brPntmlcBji1NY5ig3nx4iWkuX4TSuZvM0Z1Kj7QZoGGky9NmbFjLuaZrleCfXg9stYBqH6zupXYzeHtvhg8pg3A+AqxXKkCfTHuWa4YPMdRwHt8+bMWOG4+D2JRr9bonzaFw+hDCNjycMGT74Bh84uB1+2CjCRYuse5TrRg6ZV4Axw8l66hWDPyVRoJJMu8Aahg/qRxLau9M0pWe5xp1ihj9XRLTJvVHCycGdRP/XsZ0rgs0UsYL+sh8xHlceQGg6V8Sr7ga3y0Q54UR7wb6kIeml554YTDe43Xb4oIvLzIwKTtGhk6+4uIazY49yt3NFTDf3p+d2p4lz9cG3FZjGdjTu38hTrlCtELOvWI/Gpek9/g+YejU8U6+8pCL0knZ4+4hmMnordDajiYdT6KwrBrSsNtNhvNPwZzLSXihNGZqrnSsiZuLiRGxx4jS9jfPsPa87Pc9MRmPmTppJIoyzRdhedNbQLhnpTEbTDc0l7WB37UxGDkDFT1R3+iVvNb09Du70Qs2zFyHupPclw+xg9vPsmWZMXOMUryfHSJLuYp7R0cnqxEXyr85MR82d4p/TnX6pWBO606Ryp9C5jEZST0fQdooxtabpBneKibHzp4nvTmM7GhfdafxSERZTVsaM6rSV8Tp8puumXJExU9pO9PrsnjhKUxzDit6V/5InvjvhHOWTxJ2UqcFMp4CNGf1ZYKe7mmcvLpoCJaYwi4vWtqZiIsGdwj3PXtbt263oThM1s6c70xSjDf7GxJ1kpqarVsXvaD8P2JInziOHe5QucQF3T8ykcyffj7eXtaA7TdC2k1wr+a+QZ5SDPaXtpINouo6veE2iXLSgxDZ6wKLgD5zKEzf53Mkf5+vORXeamJk9gzziWz9mdIO9eMc+e5q2kydGuFA0NSj6p86vyf5NLneqaw0uy0d3mpipCJ03ae1p9DN7+omU9cGevu3kiYnzcKJieKznkU2VPTmp3Ck+uOx2ayy604RsO5nII8d6oxnsRevzENONiYnpul4RPOsQJwCiKT326+F3Jpk7xWNmb8Jm9jxGe/I49tkLkztFm8zzb9p24uEey0TQSztRn1IuquGZjJk9PO8USe7EsRqDzN50LT+hOQlN20k0mFg/DDEaS2xkTHQ0nndCd5owbSdj02nM3Cm0k9F0y/NOcpNJ/o1jjSn442ek0J3QnSbKaVyjMWn9aezOOxmx0rWdRN4hjrtUXIwa6E3GthO608R0J54oN6T11NbTmJx30vuSNrGnbTvFiI4RLAL1iI2OixFPojuhO02cVISlOY2+O+nwMeKl6bPHO0bQbaJxXky03JbiPfnQndCdJoY7xRjdyRMzRm0ny2BvumnbiWUgeHZP3IozuzHYdprs7lRZyK8qGS0uKJ4xbqkIE3NS2BrbzJ4BK12fPRrYecQmKV0h4uQTUehOk9ydKit2TRCc7M3Jqp5WVkj1VzxxjwqljUXPl9mbbnbCKbTPHhuWIRxJ6RHBuIqLRnfCtpO2no4bTsbzTh5dtwjrtlNWxZHkqoO5ceeL9t4XV8R+/h7l06367Al8xPknuSdEHAcr2oNtp0nvTmsL92cHdhZIN9clH6cX7cxIvlAg1TcBWPvj1kub4vbkNY5ZolzXWc+jZcoy2Mvel++p+2IDvVvLron+vD3KdWGfSdtJnGGK03yGGP6YbmgyutMLjpOJORlxysw7tEPKqCzM21lB/9XvLDiYW7cj71jh4bK4PYENY9520nQvUqCywKkWcNq7hllq1QjdiZj2Ip9u1WdPHuOk6wyl5CbQnXQ4OUvg9O//5qB/l3FyloyTs2ScnCVwMleiWp8ZTrtJrbS7StoUDcEe/EZXBRqjj0sS3EZHTx0xJO5LilGC8rd9jHZckTw9mPlUdw0FR6b+WJDBLrW7Sbfy4eI03XxI7nQX8+zFRKvTG8UPcx+NmTv9h04EFT4lqncFTtnS7vWBDQRYWs+vGE5SCqR9qWO2RfFOsnrjyQqpvnkr3MnemD9qK48fbsFx2UW2a0/EWj+mOG1aL2VQnKoCRxYsWOCFu82BDCiQMOE/zdrvAKSULzLwuCJOEwen7MyNidB2WltYf+zeUW9xwcYfCzfm+6DtNME/THDPbkJ862+m4nFFnCYOTr5HmYGHBZt8xwulwNH5ewIZvvXSbt/6vK0T+7PU3d8H5pT9XS4e1gmHk+tUxL+5zzC41igkLf63uRJNkmuj0Hh2XXLqyEtWNh9aN3VqQwE0+PI2a1f+PJm9ELneR6O4N11n9kw/a+L/r9MY4fRbJ/1ft+lvJf+9lKmXP+jmj/iDO9oHsMwZTlJweslJMk6vmyrR5Eov7iuAYxJYwcnx+D8/Tpa1b1g4TXP4i1dOjw3nujlhPu801fGHb+a06Tdnp1MAACAASURBVCZ6IXGKR5wmHk7RdiDFTKMvk4mAE/AyxWN7SyYZTuPnTnM0P2OI01Q40DZ/E8WdnBSvnm02XITKeDOq7uSRdyjcmNyPfHeilxKU/6xxslnj2OAECM3RaMxw8jjwFBk4TVOvoBHjMJ36KF/fiUHDf0PvT53A7iQuOmiP0wzAiF3tll6hc0aYcfpHFzixixQuccJpDvsd52DPo/vH/nsmCE7TzOZema7tbKRxJ6UDh+mlCUxxio4OnzspwZ3J/QnrTvLlpkOB0uI0Q7kSOyPq1Rnhwukf5/GfGfAnFm6Kk+YSuk7uRHn6AH7S4G8McfLIPx52TfIpylM8TplQ7gTPmF/NU+tOYsYiQ6RnM5V6yEWmLXHSXq3d1J08ml+5vcR2oxzvTVB3WiGu2W4ClN6d5Mu2LxRAvaoJ++S639vba7NGzasyTvP0ep/+muHEMCpZVcKu8P7SEht3oixpr++eqF4RfbTdaapy5FmN4Yd96hS5WWVSp8QyxtidDBceNIClZvaijVd30l0uLWbEV263/Nxad5LbSmKvqkhNaHdaQWEqAVGgVujDPg1OMwRNpaUCKIGDcKnhn3fiId4/sqUqoApazdxpyZJVJSXl5bChIUCFuFOaAadoK5yiuMKWimDfpnLNYD4lYhOPWWZPqU8hdcsUPBc4qTXKzp2mael5WXeZXK07xcg9dXX7KEbem9HOOEWb4yR/FOsvEsK/mwRHbGeKbyVG1FQX7vSf8DP2OFGaSjpbY8mdgZLVH4igTwbKgFP5OvZw7tIDCzVh34yR40QXumodOQcMlaeS6wsXtrXG+s8tnGfqTo3yWwdExLfEDCdqTmlpRWRpdXV1Lgl2VKclEn9UtIpTlZQhcJKHupP4KBc4JcC3YXxSlD1O/Dt16tRYkiQTJb5QTTJ7Hg+f8To+idaqpCSPJU4eD2xoAryedToDHjbQQbn8lZTTrPcePA/ENHwh1TdOr9shSdLhFgCq7q9P4H7gaFnWX4pUnBhLtFDeEf7xZ0fFktnwXNYXG9iLepzgRQJriZ8dFQVrmR3N+rNn8DiQr51tDh2NKUlf0+6P8G9qNNuWaL4tZXqc1M9tEvJp204ensGZQj/8VLZ/E5KmiHjPcN7pZdEj1j+b4fSf//mffxoXd1oBNF0Ree2S1VxK1KdrO81bKHCCHcgNaqHK0whx+kfGKMWpLZVcKy29RcgdZ5x4xLdkiVUqIi3tCumuru6EwzBQXQ04xZji1CCGuoOiHHFKEk8k2AV7Hvm7lOHkYTx55FgvxJ08U+UJ5JMoL0maumUsOQVKQuVrqGgGnPau2R13/GDuVAZWM6/QzYBT3Zrd8+F5qFvFf2mktSr75pMvNtz5sWCXDicmQCfpZGBrCE5Krwjf+aKYuPNFDCe+ltn032y6p2AXsp3Jn0/nm+Op2j+FclJFv6Pi9/JtAXtq+EujwZ00nzs07JNx8kxRozz64eluBa6SlN2sdycZJ84TxQkk+9PY4QQ0rR4k5FlHTxchl1azsI/xFILTPIbTuY6OjlskeFUbmT2HO4mFlpaWMpw6ukglBJPmOJWUt3XGBk+1tdGAj8d8ljgNkvS26lv0K4LilGSOE60pSQkg+BcS9RlwSoAqwkrGR7kJ9oQ7sVqixP9mOCXxhbJtmGqFk2cq7eken1B3umlNxlTP2u9yp9Z9QW2KPUHNA/5NmwbPx6bsyJg+fe6eXfOhUu29fwQImT69at8TM5xi9q7ZRFmKijHDKQUe1H2xge4ktvhYvhYoHtXwlwqGk1g7rNYDmyNwSoJ/SezJKHgyOjpuz64WE5zE544Kifo0p3F5CgcsiX14Gvp5KVZy2GfEKWn27NmwZobT/wFRnsYBJ4iJuqGGVhf1Xiop6YGwb+6zEsGTOU793uD10oVtXV7iY2EftScjTsFHZ89+4608e/bsoW227qTFqYO6n+/6Qou2U0l5pzc4q7y8vIetulThKRSndq/vp55GcpfU9fQkktlyuC+GtJMLBVJeEx1MSDu9yjglxdJgzgInwRErCjc0QAvBSXyZCneiRWNpkKIAZYUT1IEE9n0d5bHCSV4WhFkkofZwKvHt2c1eSl/Dgr29FKfawy2x8Pzs2dkb86FSvdzwXT5A4Z9edfjJX3YWSvvn7wE3zt63+L4U2PWE0rJjE6GTuTTuBfxi1tYv4zjRQVWNKTQYrJCkg7n0OwcWnwQhM/0XT9Lv716T8f/aexenqJJ1wTfdFwV298HqM7q7q2ZfbivemeHsfeWcM2fPzOJwu2tOSUXAhFpMB9PsXScqIBppKAhwQxREgDyaMCBAJ3hckKCVh4g02g5IY0doqK3RPmhfQWvbXr3RGnb3P3K/LzPXs9ajgAJKyA+ttWqtXK9c+avvyy/zy6QZuo1evfNsJCXn5BDitJXhBE8DG/Fetm2bby011J1StM+dlERzM13hSVd3YlUl9vCUJpAUuenBDKdMWMD67m+/c4Wv/3hqPbTT/8rzfXuYy/+KkO+mJHL9kyicZEWyZ8+ly6TrVl3jFPH+QEiLBU7+z1kIgffmXZezdtqzZ89DxAlY9j65b6GdFJw+Y5c+WGKKE/XrfVZOHt0u9/6cF3749W405RhOPKS9FhaVZd2I08lQM8cpg844kmmOEySBN56eshU1Cfx3u0iGhXZKkTmhz53OatF0l512yqBVOHOcUrDIYaoUhlPbuQnibTgxYcSp7dw2N2z/YKQCeMhM9TYMuQGn8OvKoWDlYqSltwMwg/3FraVPpoJNM7uvtJYGm6Z3tI1GYNPOhvFXFCfYlNE2mqfRThQnF8OJENfc4j4dThhnnwO3A5WmxXLACRfutnNbXHCtLfReLHDC505JV2xoE88eVUT48BINd0ec3Ept1FI7Zbp3E3Qh31sXnL6GX3Lq2YP/X7u6Zi98/cslS5yoBO6DNrn8xR4w+4KgnrR1p6tXr7La1bWLn2MUQc2X2sgcea/i2dOcFB5/1sbYozwxnPDSF74nXXXm2umPfwScBsnVr6XAw1Ly6PvdPgWnNk87DRr0tG/r9AzVoisinfkitjK9g14LU5x4pWkrvNd0+Lc1PSPdrN2JaScZJyj/KUlJsdSdmLGXZIVTBpqDyCYW6Mw2qPDb4ASFLtzWWp8JFaZMqmRmdgR7u5OBD39Tc6CiuWVsegKguVM5Wp9e3BpJG7hR6j9WCJYeM/aKW/NIzY3jWpwIvUoG4uTeOnCjIww4bYvCadu2VxXUtxOsGJ+QcdqWMvKitTQaJ7nOmO5iD+824iS31mGFiT08EOSyM/aUuhPg1LKwMEWKZfW0LjhR7QRmxHc/zwJblCcLnMjVW2CezV76eYr40dozacbtmpKCn5eDchq0bcZdAk6/UXACoG4/gEvXlVhrJ6Dte3L19l1y9e7uDBmnHDmkPdS8rbhovFb27KGpl87rRjY4wR/Fidp66ebtTklanLh3T+4VY4UTGI687mRh7CXxMpeRTnHqHLUw9kYn3F4MLwTjoLc7vXM8JzOIxt7OZHRFBI4VQvmuuVG6c76pbBh21FYVpnd6xsbGWktdDWfnRyMMJ7ap3IgT2MGIU2bOSRwPwDNarhp7o8zYg0zjMfewgI3M2EtJAZbNcUKDGTOW5XtKdI9ylqHywys4cSe6GU6+TLByAad7CwtQlOKLU21/f/9keczG3m2g6PD3WMB8jyxxonbZBNZ2HtDnCZ5mzgiTXhHhb0plm89789pkxASnLLVCdjtPwSnbDqdbQNMDOn92V91hU5xo5QlS1pNfbv9/rif1uzMV7SSHtKvaKQNfKK058atlWhl7mVQ7YR2KmXEZZnWnFJ12ymTOPaWLjLmxR8tRijVOzBFByx/FKaO2r4MEqCtCj1NtX6kbtoPN4wJ+RiqaMw04QTmfG89JS9s51wqG3c6G0fLi0Qhky1ZXTe+Vdu6KKGaDZhiNPXTUjFBXRLpLr51q+6pTRo4VUpxG89CKgwXciyuArggLnOTnZr9i1JaO6rPHlJP68ApOrHtEtLEH7zBDg1NtnHGanHr1dNgVqyuilBw8fPjChYeX60l4NgonjStidooM1IFOe3TpgStYZ47T/LDL/3mEDHzpsu9kpPfs1QFOsnKyxgku/cslMEsBp/1WOIGaJd6vbn8NC8SJ+7OUkHaoO4UGed0pg/LE32v6VhtXRDozCbdCLdqFjgOTulOS1hWRnsQbIG1cESm8WdMOJ9mdTxhOIxUnpDmo93xer+DUVUEd5XR75ndJIy/PTkCZjsIpcOxOYVrXVA7FCQy+dqgoJXVNbQVFcqaU4wSbpJEpUEjtT7rg/wDYGBldyM+2rV0anAY+r+c4BSpOfAyXTdm37VXPEMnYl46LALuXbV9Eul4a2p1S1OdGnOy0E2904g+vaicrzx5z7AFOP/34Y/y102QkEANOn3xPfL/cvg31+18Pfz0RvHABC60dTqCdWuqg2nSL153McAp8c/FiNVB117bPXlb2knAqwTsDDUqCs9Z1J+yyB9YeXDxw4TNc7FaUU9oOHtKu9ewNojVD605Ai+ra0+OUpDjKCSRiVa2t5p69LRqcUhRHRJIVTnKXCGtHecoW2Z/vPUnDcNOx3XQwpbisOodtYNurk+n2nSMnPaHF0r0n26GA+fU4kbYz1Wnz+PAUnbkzx1uaPGXTcPHi8aS0ILa5ek7M4ybJ2wbngv9P++TT84uBHkec1KsTdjtdPZ7QTB7xs4WbbtzG7sXMUa55bsu6E290QjOPLSRZO5m1O1GQeN1pVXBCY6/UwdjTNOMepHWnJ/kT5Oph1pBr1YzrvQ/aiVy9LNG607sr6AJraMa9DOvZljjtZzjxSwcscAKePsKGXGxzwrYnDU7GTkbMQ6717FngpG3G5Z49t1W8k9yMq3jJk+R6tUmvCM4Q7fZAtprjlM4chNQwopoKK28pJp2Mdqa6aLMLLgbk8SR8vMMR/dJ5bkLbOw/OnEmNPbowBLervSIy1HY6xSA2CR8Ey0757QYt5qLpTDoZpaiWbYq9Zw8ykzshtuDDU02VvoXnqAlOO9FyR0c5wym+nj0w9j6WYutkBJx899XhTz45fHtKInt/aTTx7KmdjMh339bl1kEF5smjCe9C9kpwyjJ0MrpL5D4RZgEaFKeSw4fx0j9HvAtW2olWnrBHBCxcxKYLLG+/zaCvP0NLk0knIxd1WtDuRi6+FuXZ22KGU4r8ixrVZ48bPfwX222Ok9JjiZmPaJumm+OUzAsV4jQ/sw1TZuhw8lcUphlwSl0aTukZxJ2Z5oSTO52uZ8qd9ox99lxKFxCWr1btTlQruVkuupi1B1DxnuX6PnvsyXfiq9TgFGdjb2ldYKmwbhF//rNlF9i63Fxdf1XTdqdY++xFdYG1DtBQIzRK7HpFyDwtuUe5vivsMnuUy73JlYZ+NUgnxbRjq3kf1yg9pnbD1neetewCuzM1gzXEZKg4+XsW82IfekXtAstHq9V1LTcLbt9m1QfWpEe5btWkV0QS77GH+blFzlSan6aePUMX2FO8l9GHa46TNkDjI7Zq2mdPE6DBO+zJoRor6QL7bla2UWyicffr5TcWjnIa7gQgffTfPqI4rV1wu+qMUF5/ktI3Ok7xTibcRQdoMNcxeo8zdy4pGtc4VoQGHyNNy+5Rbnwcsz57ssvBZMgNDpotTofg79TvT61v+CBfM+tRrg8f1Jb+t1bSBRb+ceFBhFlZcmSuGU5qUK42iNAkuJ3GD/4t/VzDaFw5+lrzW8q7nqWY9Nlb1fBBWi8HoDJ3RuNkETgoR0EZRjJS41sMNNmFD+ojCJcZjZvCW5+MOLGcto93OrWewe2I1J/+zNb+ZBrvpAluz9bFoL+1Iu2UJUfjIlb8u+1YEft1Cyvt9Mf1CG5XXA4KUEpwRtI6BLcbIp/0ARpyfJP+j20lepz0gxdt2+YwklGcgtvlnnlJRpaSYo7GPZX4Q69QgN56ly/UcFwTnOT+rwNfSjbGHiKUpbCUpRk0YmUDg63D0CtKzGjSFt0YEesV3K4PIzRop+RtVtppW4KMs5ciZ6b+/8YZyShK3o0aK0In2P/V+/rajC1OWasxzh7XT39cY+2UskUzQESKbqCDRBl6ZVuyzrBLi7L7dNpJMyrYmuOkaHuFJc3XLZtjnD2dYP9Xb37QSTvJWGVpTb2VD1v5R16JWtuRjHQIJW3R/pwmyNAryWl6a89mrIg0zTArJkyt9rCVapSG3OdINv+SEnpgsLgOW6lRToMMKsm6GXddRoGtrRqfYEGlcR/JSFVFW7iuSlHtvbXAaaC3NDn6W7C3mnXEa9cOC8EDCaeVbdqxIuDQLtxloZmWgFNXU7spTh/X5+zD5Qj2ljKpO3Uda9+yRbX4dEPAbtmy6XDi/V8TD6eBphNJq4GTEnitWCQpGk9UvD17O76pXipO3telUUyMfFOtG9NoG9dOcOgO7S47nCChTQ7BXlOc2oaKFzHKpHgxEoUTHLMF/8u+PXU4KJahyjk3D068/2vi4cSNvbjjpBn2V6eieCGIM040vn1pOJElzKABh8bsiuDzXy/N2Bt51tw2RJft0eoWHs6kySlFWeuSJ4xbS5y6Ch7Xrx9OvP9rAuHUieGDoUIw9nawMHecqz2u2ilFbn5MUaw82bUbhzHKadx5UsvYYNJca0EPhp7T4HTiv3FlbGx8RzJ885SVJtNkyfI3ilPlnaLQtBSoKAzSpBNdz4o8raXwJTRcUcji2dO6MOo9h+LEDh1hyUOTV8ZgN09Fj8GUSYiTH8/DbmWeDmikHNCdQs83kYKzYwdwVWqhIzDJd4Adbsuak5IGbpSylPT8hMXb0zNWFG6hJ93CDonQvOxSrnicnm/tcAq/LpiS1g+nWLrArhdOPMwd52qPezOu3DtGHmFRHmhxxTjxUPSchtFXTYVUO8mR6JVDObW91fAtp6VXjljn3zhO43nzZd2IE0s6UhDpqhgKVk6nITNKiPuTKaqdMEgDDh2hydPaQs05DePy1fEYnhIyyVswEagYQu2Eu+fOlMIBKeyACZoqheJU3Ho8XK+mmBjo7U5qWXx1DMzVnIahJB5vj+fPw2s/yUPtxO9MPYTqpR30zlE74cPTkZvWCKeugpzX5QInM5z4zO3btqXEvxl3izKWcpKGqDgYe52t5fhbnhQ8Br/uFKdOHoneW50MRbqztR7Nu87WSDIk49+4sdeNEUyIU281hgXimOQNOGBYGi3s5RjiTqPeKU4YVTvAcIIUxa31aW3n8OqYCrfwlCyTvA0nECc4Bgc0giul4HArbecmMFUKw6l2bFjCsyaxFOzex/FZkvArpuRPdxyD65mxx+5sCztki8b8y8ErYjBkHs4SvIY4hQvWGCfNaBAmYhwrYt1wOodaaTXqTuqo9NEG38pxYqHoUIkPNbO6kxyJTnEq7ByNUJxw45lS/k2pO3lPqjgVjrwYGysa4jjxA2jUO8UJx0pScWoBnDrPyVfHLTks5TYcsQrPgzjhgEYjFe2wO6UFcOo8N5FzE1IxnLzzTX3NkCKJpUgaOVbYUITBVRNJc+cmkmhK/ix4bQUnOGQLO2TLCMfpY37FQnqX8BuxdsZeweMp1zq2O8XSBXbNcWqg2qkBUFoF7ZSkVJ64jacOvBIHzx4AQpcDvVdgjeLEI9H1OMEiGYeO0OMU6ClUcerEsYtknFiIexqNei+n2mnUDCeWCrfgEGuQEjIJzuNtGGLaqZRpJwWnlBRMRXECHTbXOtdayrQTxWnk2SCYeTiYDD4SpJyjT0fYeBOKdipl2knFqa21OqdhiGmn8jXVTuvdjJtwOLUUtT6twuD28fmi1ourUXdKUS09xQWh1KfiUHea2DeVNPLsxKtj7fhD//ErFonOcRrobU5uK6NVqK6pZP6N4zTonTtzXMUJK0E9Mk7sABb1TnGq6W0mcKgeJxYIT3HqmkriOLWdzYPz8Fuh1RwVp66pibnWV5/Xw2m6pqTOVjUF4hR8nv+yOylpHiFiKenTkZrKaakrgmfcp9adtDiNlrMr7l3rupPAyYDTyDNP2WRlO+D0MQtzj6tnL0njeZDrS+qED/Fod6Jx5xP4Kz/fV53T5unrpsHpEsdp71zV2PMr1ck0WY78DaXrmQe9ZipOwWOhvqdy3SmNHUCj3qmx550bw0P1OLFUSbiFp0TPHj3PDrwV2IiePRUnmqqYUtmCq6Slknr2GE688ewkeslpSvZ0EsHzDOLDDaJnr5J69jQ4BZUrVq+xZ0/gtLbTpaVoK0+amVyT4qSd1mgyTxLnLrAjchuRyQNRb8SKZm4XOG1UnPQ9nlP0k6WtcbxTAuE00DtoidP8zITASeBkPjeuBibFZ66GaawLTsFKHJ6oPVacWPLCGHDSpHTostezGFlmvJNe+KNsJpyWPPvghtJO2iACzVSevPlps2qn5YcPbnrtlNjNuGtQd0rSopQkh4/Gp90prnPj6oJwTXHS/EVNj7sWARrG0EGB0+bCydB0q1Sh5JmK3jTtpJ0G1zBvOwNr1aNxU+QRP3XfBU6bRDvJGGm8EGoP8zcCp2S9dpLjB5UwQh1Rqx0+mKSpe25R2NpcOIHwGtJV9o19eaL9sjFxSlK9eWr0k9rh6A2sO8kfMkYantJWXzulaCKckrT5uSlxcm82nJRRi7aoakmtRcVVO3UdazfgpA90ssCJz4th4qdjMblGnOgs0nTizs/rNSDJhNH43iXiJN95bK4IdZhKNRCXtt4CTnSia6GdNny7U4rG7EtRTL+41p1oKK45TiPfVC8NJ4zH1cbkqjh1VQztaDuDYYTFixFtNlKoMCLW+7rUEic1RleLk3znsXv2aFSuShV2iXpxpnQLm+g6gXByFl70Y5AltzvFfMp/dBaOk7nsjqZkCTjFbJ7E04RbjrGn4AS4LA0n4wY1j2pvlG6jE0aPPGuPziI4zjY36fRQy8xNLU6GyNziURq0wSe6NtXE64LTJpHda3Uht4Os+AJ+JdKVTq+JRk8320OjZ4/T0Nh8DFTNx7Xjyj5IxsN2j3XT//yrGvl6nJ+PR/aeYFGnfFJrQmpulKsBtc7HqTdyXN1peuf0qGkJFqFmzXmmJfWsoSo4zzM6SzbtPo+L8LNCPsXo+r5ygdMbLP7KdtIZasb5bwO0t7X0hM08jKu1vcdpaGw7aCAWJNuu7HuSx3pfH5dx4lG8bB8ewM5Hk1QOSTW9HfRYPguv5G0YInJAbSzHqTei7LS4c9wx0NvtryzUJoUtSpxxIapUwmbJpodgl/OBJoGTwGmlOEFpxSCfznNYKFnYKhXcWNOL2ggKvp/ZYIgA25fHP/3HCmWc+HzSbB/HQk4CF4EtxVWe1nIZpyBs4wG1TsfJt8RvRLPT9M5xRxjIo/uVpLBFnvGan5XNkk1viuD4EWPdAieB08pxqlUKJQtbVYwywImFxmLpY2vKPsIjVxWcdJGvHAs5SS+dedf78b4JxdjrHAesaECt43H0muqNaHaa3jnu8J6kOGmSwhYlzpjhRGfJLqc3hVJ7o1zgJHCKJ058mnS5OgE4sdBYWorpmqK5iBy5qmgnXg2h+xQtUy5rBxmL2hvHcR30AlU4GDEb03HqjWh2mt45xaVH0V6ylusplGe8lnUezpKtDCMUpvPTJxhO/9lZWMJ/iUGWevEdzrLUlBY7d0e7A9zOQlYtpXvZKaFsuaFQulmhrIHKShfrq13T2+xuK+vAWk3PENRa9rI1ehBLptSdCt34n80nzffhAaxG8wEm4VjgsYGKEx/MtZZD0Xa7u6YkGjFrcxzOG0+vqd6I5qTGO+eP1Byeo0rIrSRtBm7L+R3Ss8J5JJwlW86Hrmej5ZBHFCfT7NttWpBWG6e/cRIZp985yr8std3J+Rl3LDXlDuefKrduYeelI6uWMgYPn0VK/W88C1tlFRUaPdvBQmMz2jx9j+ka+zVnyZijzNvgGcf/Uosm8hVnla5WPXQyTngsnTAaTC90ELKAWsfjmD9evhEaMTvo1uOkuXN/pQcS0YPl89AtbiLHGYPph+chbWe4pxJqcTgPIJ932+2snTYITm6BU3xxWqfbrLlxfNVu0899gWpKtiU6JZAY88U3JE5CO20MnFpmpPXHyW+sKCU0TjiPZ5xwsrmiwCneOPlZTKxpSr8SL7t2t6m7pm0esZTTMeKEs2S/KTj9WREnnOhcnm/97ndvCZw2j3Z6825zXXHiM03TKaZtcVLnlxY4CZwETqY4IU2fUIkCSo8TYJTLBNYscIp5rAiBk8BpI+IENH3yyWEU5Okjnc2nw4nBVFcnA/XWW7/LjsIpZhE4CZw2KE7/rZRtCNR9orf5DDiVsMmivFcXKE9UeDVq+Th5vyigkj/Bv9S7zHDiyfIjLroescPJN4KJ90mOOMnNfi667rJ5rXyvPpF5AeDNsD621BzgNklo3tPc4jbdMZQ+h1MStYVYeR7DQ5mUUzWfdGlNblN9cKc8ig0nt/YV2eOkSbeeOH30yWcyTrPM5PtI5kmL01vZuY3y3GuBBdXqixdOBQUTOOeHA050txNOXSwln9vKCafioiG3Skpx0Yk44OTi59YdYIWTK2acYrt4LOBpf0PiiZPy4GuOk/Y3Z91xOngBpJGZfFiHisYpm+J0fc+ePQ8kci83VwFq5TjVZ2RkjAAoxNdVoE75EYUTJMv5AqlzwAl2T32AJ4zEgBMCNKQpVPHByR0jTkoZdMKJftLOa6yPgsXFUTO4YgFPKfqx4qTPB2vq44wTeyaXs7Hn49lNEycETsDSZ+XhBxN7f5XVkylOs7OwqMu9cFki3oOnOU9GnMI3L14s5Z/OOPEF00ARS5zwvLiA9X2QNOIyxylMafPty8fProLd2o51JpAoOHFd5YiT/vffVjvpflijcXI4p/HiFKfwyXZNrz5iBp4KatSTa3Fy667ttsXJFSNOLj1VLiec5F8KtyNORq3rtnpyxAlqBSPKL/NazsIX3gAAIABJREFU4vRnjtNtytNn5bQKZYsT1U51jVPE+wMhLRY4DXwp1XwptQxLfPp2J5x8qEwYThN2OPlA87hkw6/eHCffK8jNj9PpKth9GpyCxzyh55VlHd6G0NNQf5Vn8aWnrLm4qK8qdCLPTadxoDh5G8q6rcqpy6GcysXJtwScrMq+HiemndwOOLmMFprLGieX7nlc8dFOPreiJ5STWuPkM+hHJ5zcxP4nh57ZvZsZ++uHE73vbxGnq42HP7E29jgst+ouXP5iYfZ7EgT19JYGJ3l+Qf+XeUDUzUESuKjp8KWZfTC67gRVHQdjj6FCcZqSMK1kXncKs1OC9kJltlt9eW2e59dmGjztgYrWuaKya5We1qdF54pxahqcQ62sv7Ksm+J0MtRsbcP7WDm0x8nljsXYU3AyP6fx4jJOxAontwEnYpdSuT237cX1ZDri5DKc2cnY40/vaOwZcsh4cZ8ep3pX+IvEwOkROsxtcQo8ulUHMnvp5yni59aesRl35Om1/mrSAjrqmsbaM2vGlXFC0y02nCRWdxpRFFmUo9y3I5+ZjZBG0uG0WEpqq87VVI6DiYfU+JtG54tOuDs9Q22eQgILZuylR//sZ8CfxppxOXoDloKT+TlNcPI54eTWW2jWKV0+t74CFR+cuPjMElrhZJebeu1keXEtTj73bt0vc3xwcg087Z8cdMVo7F2gTU+flQNTn5h69rixN/vARQ4iTg/ouIFBc5x888Mu/8VyqDvtvgj2o/fmNexTb4VTPZp69bHhxI29CE5VaoGTL/MDF1VRUxLDSfn181d4PCcCFWdehAoRp4ZQt7+nFetOAFEDaCRYxFB38jkZe66l4+RzMvZ0OPkcjD23W3OvVjiRpeAUW93JtSyc3DHh5LM19txGnEi8carp/zL/JqiImFwR1xvRpxcLTrOXie9eXd3XkvfRpQcuC5zI/F0084JTJPil5KidqEuvIBILTrIrwk478R1dDKeJ3dqXN9BT1tEWunPmuB6nTk97m6fdVju59ATYVbNdipspNpyszuk26BlH7WRwRTjgpHPv+eKCk/Lgcp3I2bNnCompZ89Jg8tYAU4TcddOvvnJPBJ4MeyKDSfqIf/ks3Lvr6qtZ4ZTXd2FehJYqHtAgrd43ckMp8A3Fy/edcHn51rPniVO1OSbcHaUfyA7yqHu9Mqq7gTI5U98MIJ6jNad1Pc1//xiU1lHTaXnnKTFqa+/qqyD1p1C3bVFfTOmdSel6Pvcbm25MsNJrY7YVJ5Vr5bVOY2uiEAPkBSoKLR2RSiO8nXCSf/gMbgi+C0742TIIVtH+WrUnXw3ZyTifTEdK07Y3MRw+siqVwTDCRQTLODj6mWJ1p3eWlEXWK52qLlnj5O2GbfAxKWuGHu8GRf2Gzx7c1We0LTkPQnVJBWngSY6b6yXefb8PZ7FPDPPnit2z56+VNl49rR9MmLw7HkbWqtz5vo6rHHSNuM640RWFyd7z5720WPAycmzp23GXQ3PHmqnJx/HoJ1oJ6PrtHvRR4jTR6Y4vcU6GV3HptvLJHy/7sEEefJowrugd5QvGydq7jnjJHcy+tim3Yl3MmK9lkzanbwNcpy0O9bSpzfMzPzKK8Ap2pKxaHdyj7wswlBxG5w0zTMx4ORbPZwc2520OMXUjGvwRdh2Mioo2LcKdadv+mOoO2F4Bu/8KsdpmHaBfUvtUa6RbPN2p9h7RTimWEkXWO++ffq6E9qhL4vGJadTJmzfUlv3d+Lc5rrmJq871ccVJ9/A0/7+/mHJAae/YRjx+EF91JPe2HtLjXfKzs3Wh2okKk5fFERpp2Blawd5k3Gy1U4CJ8XYi5B44kSla8pJOynBuMqadTTuWxiWka2XxA7Q2JtPcUr0ArCElPYVN4ETN/ZYtWDNm3FloJRV6/BBQwguzkMj4p1EvJOIdzLiFOtIRm8BQ/Tf7+TQwbcscRr4UiJe1hH2G5OOsAIngdNmx8l5JCOl0vL62oyESAWxI6xr4EtJ4CRwEjgtF6d84Mg3j11gsZN6S5S/XuAkcBI4xT7OXg3gdLMbLL3jYPP1Dxr2CpzebJz8V+7c6Ai/vHNjUOC0Zjgp2slPPxMKJ97XVeC0vItLpK29eFyqXcwTOK0RTnLd6a5L4BQPnIqLPB5PiPZ/8t7sxaFW3YFnhepmOpU5qTnm6WtWFm2wD3so0iRKSnY4n5kTU0Yt+MlUbSSfelDe1Nbe1g7bj28anAKvHz+ecq0jTsyzh91hE8/Ye0O1E5v3CHvv0RRtbABjN25mU5mHnw1Jc63lfEHaeA8QNz+SpmSHB5uGvXNnygMVQzhXjX7BT6a4aek3eR8DrP94QyEJXOnYRNpppEBaL+1kJuuMU7DyzHHvydCXV4o8fTTsttPTTtpChdj7ta9ZG9OesDjRiZ9x8jBWqGt6m2ihx/nD/Gwqc5wNDWfBZAvSxqelcfMj6Uxj7HAEy3+sGedE8/cU6hf8ZIpuot/4vvk7z8shs6bJJtNOJKwf8Wez44Rdyf09o6+u9F/xnNPgVFvV1195plwTl5GwOLHJnOnE5Wh+PJtmhZ5tpvOHeU+O53Uu5vGFihOfBhoX/HA+BTqfsVO/4CerHesmna3yxJnKPpB50HrFi5ur7hS0MfVWByfNaBAmYjZWxFoae7U4MsQQjglEY9plnNBiasMqRXrCG3ttdJajYO+dIpy1bG7xY4YT28xmt/T3jKHy4QuoOy2WU7OQzY+EC344nwKdzyetX0iczYbRV3T6aPpN2Qc5WXXnzjR69ro3j2fPW1C+1q6ImGVdcApUnHlZ1tH1cszjOavRTg0epYqf4Djx6f1qq6al+bHumhsdYUoQ38xwmr9xsXJIkhfAXgVWn0Z4Elzww/kU6HY4gTE4Ni6Z4JTYDsgN14ybmDgBP0XnpIbQ9KtKBacG0E6h6X37cAzmhNdOfJJmaqZVtON0lh4PrPPNAbnuNNDbwRfKQfKRdJ0dTsG8UW5n7AFCzACOMvYETgInEqwMFUINavKl52xLUd9MbVHr0yoP1p0uPp2REr/uJJdlOqM68uAOs+rSEFHKPPof/Mea+UKGjydhC+Vw6pjg07PrFzJONb1XzubJp1b2CZwEToQ5mMtx/uTnFaOvejyLIy89ZZOV7V4MegecEt6zF+yFGwx+Hgn0nJDm+zpknOhmRTs1TWfM3zjOF+RjEuwZUpKwhXI4ToEOR51Al7p+AdYhnix88oT/WLt8amWfwEnglNAFILaUaG2RYgAB21OHiYwT3SxPZS43zvJ50HvghyJPTiIv+OFsCnQ2PbthwU+GXj24nnxqnkTgJHDaCDiJ29xkOInZBwVOAqfN0YwryqnASeAkcBK3KXASOAmcBE4rxgmE15Cusm/syxPtF4GTwEngtDSc3AIngZPASWgnUU4FTkvHyVk4TjHIUi++w1mWmtJi527d/GXsHTgLWbWU7uWmDFTQPnplBb0diXybCZCbu00LkpB4yO4N9Cz+pmb46O0Qb3XTvHKRt6uIE/a5EzgJnBIib3Hm9sU8OpGTHOtUHOovOoF9YPuqTWLcExSn/irPuGTonHfjSqjphMRHhBCvXMjq5y2duZ1P0S7jVBTqH6ytCj1/ftwkxj0xcapcjLT0dgSbpjPaRvNwMXfmuL+yEIOZvA0nxBsXOK0VToulhE/RruA0hNvb6d6oGPeENfb8x5qLW/MwuAkX/mOFdGNTc6CiWbxxgdPa5C2duZ1P0a7ByYub4DM6xj1hcQocK+z0jI2NtdJg2kAFxQlUU82NcvHGBU5rlbcDPWUv2RTtPLCdaqcGpp2iY9wTGSdeS8Jwda6dYH3OeWJFgZOQ+OQtnbn9sTxFOw1spzhBBer5nQ6TGPdExgkqTdLIFJHrTohT4NidQvHCBU5rlLd05vYM5tkLsMB2ihP17HWbxLgnMk7o0sPRwbhnj3rP2+QxWsUrFyLydqXSeU7YegInkbdxUl4VwtYTOIm8jRNNPYuiDVfgJPJWiHjlIm+FiFcu8laIeOVCRN4KEa9c5K0Q8cpF3goRr1xIrHmLM9KYT5BbW/Xm9nyr6T1u8o1HHLLh+/Vito0farVriRKn0wic3jycAt/MSGSg6cQbgJP3ZvVScfK+Lo0+jck2fqjVrhhvxekKAqcNj1NN5RvTTYfP3rQUnJav5pZzK8LY2+A4sSB2wvrAyjjJMe24r6DS48Gpp8clnibUX+lZjCRKr1jW25XN/5zf4/GcOa5Eto+NnaC9YT1lxzVR7/iNlvfKO0WhaQnjolhS/7MiT+txjIhvrijkBwSeeUJcLbNDefLQ5JWxvm5tFP2wkpKex3gr/AD5fHAatqq/WYHTm46THMROo9tlnHhMO9v3oujMZCngpKQpm+zxFCZIzAYPZ+fzP6NK4Fv8lUNSDQ13l2p7j6tR7/iN4zSeN1/WjXywpN6CiUBFO0bEwzZ+QHHr8XC9fCE8lCZvJ52hZpwRV7kWRtHLKfl5+K3QIHvlADkVnIauKinoHQic3nic1CD2Ts+QjBOPaWf7qLEHOClphugYLYkRUcjD2fn8z1iG+RYl3L0cbTQl6r1cZ+xBsedRu8w28zYMsc2F/IDasWFJvhA9lCfHb53nJM211JT8PPxWeBgjP0BOBaehq9ow/NW1DgVOa5G3chA7i27nOMkx7XSfgpOSZogUe9oT5El4ODuf/xmLJN8ih7ufzUMKNFHvWpy8J2WcIGn4xdhYkYwTP8A739THSjk/lCevZXRorqWm5OfBW1GD7PkBcirYSlc1KbQz7Aqc3lTtxIPYWXS7op1YTHsD105nuXZql7VTceJoJz7oF5v/maoEtkUT7o7aiUe9j+pxCvQUqoW5s7VUo53kwcS8c63aQ/V0aK6lpuTnodpJCbLnB8ip6Ly6sDqnphA4bQSc5CB2Ht2OU7fDfxbTzvb5K0PPu+W6U6ib45Q4dScMZ+fzP4Pxtpdv4SW0preZtJV18I38G8ep2wvVFhWntrN5wR4ZJ35A15TUySDhh+px0lxLTcnOw29FDrLnB9BUrz6PwGnYqppC4LRhPHvdXua18/d4Frvgfx6PaWf7GphnL0P2/jGcEsezVzYtyfM/t3n6qtkWXkK9c2Njz6908GTyN1p9eeahvjsFJ/+xUN/TExwnfkALfWSWT/RQPU5EvZaakp0ng98KD7LnB9BUcKNwGnaAmkLgtBFwErIessrsiFcu8nYzSU1vt3jlAqcNIf5KdFwWxj95zCnXIeRe4CTyVoh45SJvhYhXLvJWiHjlQkTeChGvXOStEPHKRd4KEa9cSEx5+8bFsGPUg3ifAqfEzNuBphM0ll3gJHASEo+8fYNi2QVOAqcEy1t1tnYMWa+tWqSx7Gw+9wSe1UngJHBKZJxYyHpt1Tkay07nc/8ggeccFDgJnBIaJxqyXls1To09Op97Is+IK3ASOCU4TsUqTnQ+9zehnAqcBE6JhlODHqezWEAHeso6hHYSOAlZUt5qZmtnONFYdjqfe0fi1532jlQMidcpcEqYvNXM1s5worHsdD53b+J79jo9rR3idQqcRN4KEa9c5K0Q8cqFiLwVr1yIyFsh4pWLvBUiXrnIWyHilQsReStEvHKRt0LEK1+a/KOz8JT/w1l4yv/bWVjCfzGX3ckaYSmTnYWsWsrkeKbc9Le5sXH6BydRcMpyEgWnd51ExukdU9HghN0h9C+ruGp8x1qX052OYlFOg1eq4bPzXE5y8sjLQtwyMlflKRuWMGXX5/WY5Ni05oCuHo/HczYicBI4rQ1OtU0ncsxfFot7TyycehANilOwchzvu+3M3R1zVYWYsnhx3zfVySPfVOuPGegdTCjtlKb8yZKm22aW0uxP4LQWOL2t/+eIk3UBYHHvq4TT8spp8NjYEMep88aNUtjQhGOEt43mgZ56Nt11rDnqRCMn5Z+LqNuUi3RUQdUVaK1Yp4xXHqUtPaXAaQ2109sGnPqqQifyao4VefoGaUx7S9U4XUZ4eYXVfXOVnr5hP417954sG4w/TrC61+7PUjsde1pWTXEaOTldAdZeLZ0NDT5h9UYBzp+eD5vncRql5CDOyp5c3FqaUHWnNGs8orWTNchCO9nglP1ejDhloywBp7ejtFPoeWWoMHil/4rnbIPnef9MC87bCUtWgWpjm3Am93007h2nHVwF7QTMLE87DZ48G0Gcam6UtsGi+Ew5JAv2difvbTiRjNpphM4luKNtNBKshFrUSAWSFdttmmknqzRCO60xTvvhLzacsrMPICXOOGUrYokT5efT7E/fYX/Rxt4JnPGWoJk02uBZnEql0+AuTvH9dLXNU5jcFurmxh7jLJVKTEUlNdUysYwThQm10E78F4N24qcMHusO9gwhTp3ndgyAtafiFOytRpxSR3Ae9kgq7MQtaO21tdavVDtZPpIupc2DW1xcn9yonWLUY5sAp/0H9oPEhBOwlJubewAWTjgBRrlUooDSaadPs7PhH/v/DiK1W31rNNCp6ETXyyqP5+wrMI7GAacgLnfwuj6snmQzuWvqTqmpsReVVJvEeu20U/VJ0L076Z9NOUWcUufLnp7LGaH3OM2NvZreDuRLxonOsH5GxglAG4y+zVTT27TQTmZptSXa5oyOeRR1ByYpN712ojQd2B8DTgc4IkhUVrYdTgymujoToLQ4fUrTHck9cuQIpnrnnezd6jvjY640hGZeV57dkfq6p+xx1XgOLmV/GKy+DE3n5+dLLO4dtVPqEoqKbVpt3UnnyWN6aiflDP9scBo5OXYuBzVTctu5HcGmduaK6KoAm1TWTqMRmpjjVMOXxKLsW95msmnht0oZyymJOU269GYpN7mjfP/+w9Xkesn+A+yLTlPpcYKyX/JwykWePEJG9EZfFE6N9fT7k285UNmm2im7rp4MnAbw6n33KVG7U9OJT8apr7+qrPqk5/lLz9k5jGkHnOafX2sqq6bvja4+ZjO507h3WneCHRluQtwZO03LgKGcuvh3b3RBULVTMtVMmXBW4suUocogPllT6cuUm5/Sf6zbRYI953KAJHSBVye3ld3Nma8qJIAQ4FTRvpfNw/5B1xTD6buPu05Gtzul4ikzUunNZlqVaA1NukcyT6nepHpGyzxy4/tIhdcCafkdWOCU5sL7FDgpOKGiKkFdZYYT6KaSy+z7QdBP9E8ByohTLseJ+O4ZbD4tTtlHACffvbq6WcCJ6qndqRn09WEjTBOdwHyg0vO8YvQFxrSDsUdj23Poy6erO/hM7g3cs4c08QvvNPtRtcPJrFAlY32J4cPLnw4n3GmHU+b84siz9lR0M7TLzbjek+2o8XD+dHke9hzACVSZJ7RYmmyCkysKJ7XUWuLks05phZNpHm1lV6dUKXdgCh7DKdXU4N40OB0oYTgBQ0BTCRWZJx1OYJc9AJL2XAKm7qlWX7YJTtkUp+t79jyMkCAz+XJNcPo0G9QSIV0LHKcjuXUanDQFgBWpzMxMt1pKtC+MaFO6MWVGVEkxptSc1dSY0TfjZqJmotfX42RsxqUnwIvDWbeq5V97yho0/nSPlGlxcT1OW3U4pVrjlGF4IhOcUlNpDmWmxpBHNCvph8UDGXBKTbbWeJtAO5UcLgWckKf9+z+7LBHvwTqZJy1O71FEDtbV1TVOfQcmXOP3E9SUs8Fpdnb2e+K/dSES/nli730z7URxItdvzUZ89+HMl9N3Z9jiBDszt3r35e8DyeAF0YiTC8tyZoYbX7+PllbTlMayR4tKBuopE5zwxzmTnjYzcyeWLZ8FTsmKYcR+193EnWkofS0zOVGUuLkGyIxWEEac0kGzZBjPqcdJLsqwiseY152Um3TKIziNL5Oe1eKBlJRu+dJpPDN9mw6n/QdKGjlOYPZNEe8PoIHMcMo+kHtbwkJfQpVNHeioNDTlmHqywAm1E+AEOwKnuXqK0k4/kMB9wAlMvsssb+21U+ZWNg35aJ7bTS26aO0EhT2Tl2fiRrvGLKVRO6k4pUbjlEkZ3ZnJkIITUmvSGSfFoDK3NOmVaWHGssx4MccJr8vv0OycBu2k4ERtXgecbPMomaVkrDk9kBlOqZsLpwP7KU6NJUw5fbHnwvekC9STmbH3tRRGHVKSW5Jbd1vyfjv7wBWsy7XEiZnwj+oApwGw+Ky00yPY/SvidDuPXN+91W2Fk/wqt4ZfPwaZ+iBTKX86nLbSioGPWVsZWAozeFG0rjtlctUQrRoVW49xhJqBntBtgVOyrqT6qELd6YgTfZKoixPDXRL+SKZ5FP1IeH0Ls1CvQlkebTXLo2R2h5oHsrhNHU6pAqcSrDg1Xnj4YIr4zXAC7cRwYi5wgO7SpYd54QV7nJ48qkOc7sFRVnWnew9c3keA060HrsCCTd2JQcKNnkzlA9PqcMJ6AS0AmUynyB+GlMvGKYPafRkx4QQJ2RcHnPDCmW7Tn309Tuk0C6LOaYVTZiw42eUR+4HiXLITWj+QwAnrToDTwcZGdEE0PpjAHVbaCYw9MMnq6h7uQZyYS+x+rp2xh6kBJ/QzZFtpp3t7psiTCcQJ6lm2rgj2quhLVT+icaIWGa3sxICTUneyx4lVyPC0S8Up0xULToiJy2eJk1J3ylB/UVKd6k5xw0k+JzvhVpfAyaHuBDgBT41fS95fLj1wdcm+CIN24q6IC0AK4DTyFcglG2PvOvfpWeLEtdOthxI61J20k66UWOOUzpwGGTqctsaIk9sCp52Uzp1LwynVUTtpPAwu4o4ufdEJY9FOBpySHXFian6rI06pS9NO7k2I03amnWYbUb4nwVmbulPu98R3cM/DKdBJdWD4Qd1p30FbnNA/npvbGEEdlv2uRbsT80HQupPv3u5MlxNOqQ7aidZY8DSZtuBFe/Zo9cECJ8VRTutOmTHVneidpLpt6k4aR3mGtopvjVMsdSeNK8IZp1T7PNJnvvxAMdSdMlK1mbmpmnFL+YZvv5bI1csSCZjiBDw18mZc0Duw6nviIgdNPXusV8R11nprg9On2Qyn2QhBnyGccreb2ONUXDREX7v60eYp1JW+DEPlQf2wdkX46GFuE7ei2guCp2SePbeVZ48pSLIzVT17pkMbcmaqUs23wyk1Vs+e8kiqVWbStVCLk3UeGXGye6A0t/JAxszcZL0iOE5Yd3ryc8S7YOIoZ90iHtQT8t0jNOEav99CwtfN250ApxLECRgCnhAnq05GufW0SfiBC+3BugdbLNudwBYbeTGTk+yMUyrtDpSR6VhUtGVvJy2oGVbtTnInI3cmR8uy3YnbmztTg8ea4aJuf4/HE1qk/cRHXjabXNytaEefaXcDYycj53anWHHy7YwRpzQ3URoTbNqd0jS/DywzN1+7E/JUYhS5256hC2y22gU2t0Res+xRzvsVGeM0dNoJu5IfyT1Cz0SXu006JsgOu5rKcxQnQzu+HiezPpsWLf7JNulWEtwud4FtlhdXK2jcRbByXLK8eLrOMovhgWLpAmvfuy+mPLJIGltn2U3YK4J11GMQsRW1054xQONA9oFcHqGRTVcPZNvGO5nFERrCB3mAxhH4j5/aAI1Qf5Vn8aWnbHgvDbkN0pDb4qLnTZ7R+tT5StiRuneuyuPxFPIJamwLSmoMwQemffaWPlaEEafkYA920+u8caPc4uLpbqJWsWIqp8k8JsOcZf3DpJmljDWP1MgLy554jthtrmjc/UaxDB/MxpAnjM54L4vGaGTbReNmxRDcTqOcMISQ4sQCNJTwwbJrlZ7Wp0VnWchtPobcVhcXee5U4szTZf2VZYO4aAKc2PRpSw+Ns4k+WAFOPBpXxik5eW/DuR0sxt3i4vqak21cng4mk2hcy8gL61PGHI1rnkckZtWYKDgN9FevIk6ookAfKf+so3HfW95YEdnLHMkIMOn2YyguhtwOcmNvPKfTM9TmaU/mC2rspa+4qMR9JCM2tgpbtI1GkmtuHG+j1p5lMU1d6m3qQ9bT7CNil4FTmv1wEbHdpjblZsHpPy1hrIh34zT0ytvOODUATj2tLORWxmkoudgz1IAjlRSN48JQd4r/WBHLHcnIgFPnOQmIsvvZt7nNNNNCmmw7VoThyJXlUdryBmmR9yQkTv6nMxJpmSwNXCv9pr+//8uWGSlwrVq7OXyzv//z8paZFtg9LAWf9k9W+58OOuO0PiMZvR3FlClODTTkNqem8uwOipOqnajeWl3tZD+Okd1IRipOYOzxGPfCJd+mPNpCmomuMGons/GEVqCd9IMRpVkpPGKnGhNZO7VMXislLf0zI7AIXisnHCfN5vnJ8vDNmfkZ2BO8Vt0yGRm4+0F+JFFxeucdw2h75ji9piG3OcHK0PNBjhOtO4XgW+vFqLpT4mmnYNN08sCNUkI6lzscYJr56ERR2slsoMm4aaeok+u0k/WYlQmqnQJPB28OSy0zL76UcQId1F+t3Xxz2EVqJ28iTuEXg+HX164NumIx9hJzFFiOU4SG3O4YafCEhjlO6OwrG04eeYGjh7XrPHsJM86ejNPe1zggbNu5HRg62CG0UyLgNPjxxzsGAJ7J4y0zYMNptZN2s0Y7+a9Vv74rgYJKVO0km3pvv6OuJNyQ/zt37l2mdsIhxz0ncBGajCSPPGuHhIGKdqGdEgEnRObFMAm/GAZSWnQ4aTdH1Z367yZw3UkZrdJs2MoEwclJO632bQrt9Ka1O62nK0JHVEJqp1UYrVhoJ4HT6mint9/RufgSUDst07MntJPQTms+gwbKXzRkCe0ktJPAadnaSUbpLwlr7C3Xsye0k9BO6+SKUHx7G8izJ7ST0E7r4ii3mN8pYbTT3mTh2RPa6Q3RThrVlLB1p71COwnt9AZ59hK63Wlvsp2GEnUnoZ0SyrOX4L0ikhWghHYS2imxtdPb1n32Ek07WWkooZ2EdkqcutNfGFN/SfS6k7WGEtpJaKeE8+y9nciePRsNJepOQjslYLvTm6Kd9grtJLRTQneB1azrlh/AAAAY8UlEQVS9AdrJqKGEdhLaKZFcEW8ntLFnpp32Cu0ktFMC1p3sonETWTtpNNR61p2SY9JO5uPsCe0k6k4JpJ32JtRtxjPlMrRTstBO5B+dRcbJWWScnIXjZC4Jh9Oql9PNdJsbGqdEFJG34pULEXkrRLxykbdCxCsXeStEvHIhMeRthsiDzSU5jzfIg8Tur1sFH+Aec3lckKkKS7muvqidMUgC3KY7Bok5JVm9lCZSsGFwes9JFJx+4yT/uNRzWuB0aXfBxwKnpePk/LbdsaZ0k9VLGa2bCnbnCJxWDac9lx7vFrJ55PHjjUJTYuKkFZZyl7Pwi+9630mUlL93Ep7yw793lA+XeEryl7ed5C88pcW8CBr5F5Zwh/Pb3hFryh1k9VJuZFlFnLYrH/HE6bz8L4FxMlxQ4LQ5ccri/+1x2v8bnDoXFw7a6cB7B0BgEReczuPf+V3aPx1bBpwOMYkFp0PxxUm9+KFoosxx+hT+nHHKfgfnDxY4JTpOFKEsWvadtZN+QmobnA6oAkpqO1NV7N8ytRPyJAvjSaOz9DgdOvRXKiZEGXBiBT8GnE79/SkQWNjjxGiSL65QZY3TpwYxx4lOw/0pTnAvcHoDtNOBA9n0X5aqqMxwogwdLjl8WOFpvwVOQFEJFYXS7Tba6dKeS5cuKZ+mOJ03iKqkorQTLc5HQWiZtsOJl3xznnQ4nZLFDCgdTnhKfnEZKoWnaJwAoCMgUTwZccrOBTmSC0AJnBIep+wDmqKfZaOd9u8HlhobD6OU6BWUDieFJnZWvdFnop0uacRCOwFCR5lEUWXEiZVnVqaNCkqPE+WOJlI0lcJWFE4//qgB6pQpTpSmo+rVNTrSFCcGk1Y4TzqcPmU0oWRnZxssPoFTouGEZX+KhBcoT8xAy7LQTsq8a48+qyffHtYAZcDpcD399uRbzpPGlozCCRiKkIPw+VDyPTLHCdE5Uk8GTh89Wlfv++molqdonE6zi3fd46xoqjJanJC7KRL48ShP81f6JxOlwQlZ+uoHF5zwlE44VDqc5IvvPfjj0aO3Jnw/cR1phhPS9HDKRZ48QpJmp1y+60dMcMrOrqvn31uOoMWXnW2Bk/eLAiYTTjhhSrgy6YLEfG7KroIpyQwSSIo7YBFxxAkS1bs2N05Qbyq5nUfIdSj5YPAdyNUUfmucLiBOVEWZ4VTSyAuA7x5TUSW8FmVu7D3U4HTJwtgDjuBsp0/fQpw0eooCpcEJIDmtXNygInQ4oSL5FcrJdTnRUfpPtv50OP14mRfnUwYx4HRIwQnSMpwY0pQnA05AU6583tNHTn8Pvz7XuXrS45Sr4sSMviMqUCvAqUAivlcx4YRJBE6x4YTK6XvMzjos9rms+GczBWXE6XDjha9d4UsXLjQiTmj2yTxpcTpAcTo4OwuYBOtUq89SOznidJ7hRIILp29FfD+Bkjp6RAZqlxGno1Ciry/s+WqC1JxWjS7GkxYnoOcBrAZ/xCRHjx7VmogGnH4G6u7fh7L/E7X6uHCetDjxiy/suUzC908jTqfpCS1wgusf3HMJzgu/E5cRKkucru/ZM1tXR2FiVp8FTvUZKCQmnCLywhGnfEngFLN2wsL/i+T9tg5hevAD8R6s42U/qu50uPFrKbynsRFxenRZ8h4sscTp+uzs7PfEf6vxwmUJT1miP6clTpestRNBTCI+KKeR8KMpMnJP5skEp4WFy8S/cCtCQD9ASaVF2oATJoTnRmV3Swp89QNYc/hxH9JqcTp16vQEaUF+pq7+9COk/FZO+VtLnBZ+lRhO9wCTwG+BZROcjsAjtZw+fbpu6rt79Om8901w+pThNHurjuJErcPrin6KwomV5vAXBR+jVhn5QlFV0TjVk0ABowpsvnw7nOC0DCcfnjB/whknWNtXoAK4ibRTScnXUuDXKXKwro7qqUwXCeYeMPfsaXEimVsI+ZarJ1OcHtaDdmqcIt4f4FfYGaevbLXTrXryAwncB5zuAU5gGf2A1pw1Tl9FQDtRnPCH/yhTTypOaOs9lAL3p6BEI07EdxXuEj+CP6J60uL0KzAnqyR9SuTJQjsFgSnA6YEr/BOyHIUTKKcLEvw0nKY+iDqgxPvkvmndSdVOdXUXJsh337kI8GSjnVyIU0E+coAfkilO+VB56sL9EV8XMxFtcCqYYDiNsJSRWHDSGp2bBSesOTVeJlf3PHAF9sDbipBHdbfzwgus7Edpp/2HKU6HEafg7IVqIqunaJxY9eURKKcv9oCaAqsvNpystBPg9ChCBn4FnBZuTZCBhVtQZK1w4nUnitNphtNftThR5YRaawGeewFqZBJA8JB9hH+L6kmL01eABLXuGE7Xf/yVfYR/a4oTlcB9itMvEq3BUWsvCqeHqMIYToqx97a5dmJl9H7d167grdmHv1yywomX9jCW63AB+5gwxWnfFwXSK/yMsMRfWONUD/soTjSR1yqlAacpKcO16bQTlP0LEd+j2Yd5AFId6Ck0KuSaTnQzLuJ0i+H06MKFu2TAFqcnj+pAk80+fDBF/HX6c0bj9NVXTnUn+Kn3PkKc9kyQewtY8heOWuP0BB0XEV4tMeC0C3FCWwyKPKYA/QOrEn6Xwj8dNcfpFNNO3p8w5U+I00/WOAHveG6s71nj5JJxOm2N0zs6nG6D4fzdo4U6ufZkjZP2wwynCP0HJmFkhHolbIw9TIHJUTlNEP7piFP9Jqw7ZaGtx39EgrN1XxPAqdEJp8OHDzOcvrfB6eDsbF1jSUlJ4wOa911OOH116YGTZ+/eHqgwTVCc4IPWT45aGnvUDYE4YS0qSjuhrffAJRf803iqBfkjCifZ2Lv0W8QpzEiyxgnrTl9tgQXFyUY73ZbQV3nkyKUFGadPrbQTqzuBPMAy77tuhZNad3LEqQvtvQ9knOxcERH0AHKcIE24QH9KC5wimxCnA9kljdX8e/j+LGinPXWNDy/VOeGE7U6Ntjhdb2ykHr2vJe+jSw9cdjhdqidXv/rqqweY0lY7oT1GmHa6bqudrp+mNFnitAv96VPKc2twumWCE3dFLEyQToaT8mGJ08IUUAo4BS+j69ACJ+6KmKX3Czdp3ozLcZplONXNPrwMdciF3BXjhPWgKW9M2gkJKliqdtqMOL2HjU7eb2dnZ0HfXK+7DXoC6k6++1Y4lVCcShhOjbY4sQanEqg2oYvPGifg6TLxHnz0cz0JfGuvnU5DfYnj5L9P604mOGHTz3XmIGeFG0p1tHb6619n0cBbQOffdcTpp9O35A9j3enUz8R7/f79KeL9SY/Tb621E1yTevbQmDTFiTnKfQf3XJpClx7H6W0r7cQ8EXUPUmpu3XooBRZWrp0QkXovqztFiPcLO5x8XbIN6Vh3ysDgW9fm1U7ozYYX1Ui92t8zsy/XCqf9FKf9JZ+VWuMEPDWW0mZh7G30tUSuXpZo3cmyV8RD7gI6eMm2VwRYRrMR6mGYkNtpo10RhxhO2NQEPAF+e13p0Z492PeA+H88Ta0s/48KSUejcdI0417/0QEnTTMunhDbnfAyVjjVyeeF6tNlMn/EtM+ephk3ePp2HnnyXTrtHrFSnLCmRR12yEq+nWcvQk+Iiy5dM7EZTrz2tklxgrpTKTlIG2/Bkr9PazqW7U7IE+KEHr5S7BVhidNhxIl1LiqBMz75ecK7YOUoR6C+msog5MlBQx9YVTvtojj9dPTo6QcuHy2nSrtTdCcjBI/1LvrrX29ddoWvP6A4va+vO0GqeWoQPpR8PzGS8tjHb/WOcsrTVz8Q8t29H0+dQogUnP7fU1adjMh393mviFt4N2Y4sU5G9LxHGE7mXWA1nYyCp3MvQKEPHzyd69ju5IgTUiQpuid/xBYntPBianfa3Djx7qq5B3JLNHLAGqdoMe9Rznsqqb1hD9jhZNoDVhfvdJ52gqV9IY5i14j7WDs6b4bTIaUXxCGlO2xUrwg5iOOvf1WT8J5GUb0iWIdy3gU2upeRVRdYTVfYQ6Y4abvAfsr6lZsGaKhdYJVeEbmfZosusImIU1YW9ijCwk+DNHIPYMHnfYzMonF5ZIYx6sk03kle4x3LbcIHTWky9CiXBZCqi9COe2Z99ljEEe+jp0Jj6LMnR2ccOqTlSg2qiIp3MhfHAA3NxWMJ0DAPH2RdyoGjI7T/K+1Yni16lK9IWvqHXavTKyLrAPzPyoKCn0Whwr9Ygtt1AYRanLZjPMYBJczJqUe5EvRkEz54XgcUx0nWTdHhg0pYxiGFmveju8Ae+v0hJSxDld9H9ShXgHKMxjUJHzykhjyZ4iSDpAvKNUbj8uBBHkb4qSbsSeC0LAm/6J+MxB+nLPyXxSPb4S9LDXXH76Y47f+NGja433rolQPaJedr+3sriMbdtSs6kNA8uF0nukhzq7EiDsUU3H5KXZ5Sv1kEtzP1+P4hNcLdKrj97ZiC2z+Njh0UOC1Xaq49vjZIwjf7+7/c8U0/fM7PtEyWBq6V4qbPy1tmWmDjsBR82j9Z7X86uATtFCVZ8RjJSDf2yoEVjhVxXg5vZ2sqTDJndjjtWrehV37//u/5Qgy9klg0eW/O5NyckVomIyOPy0nwWjlBgGZGrpXOT5aHb84AXDNS8Fo1JBi4+0F+JGacsvhgEUwfKTDxzcvCabtuDCPtcEbblz+SkX5sCBkms+D2XTJCu4wsiYHBBE5M/E9B+fR33GT1J47TzIsvr5XiptrJm4hT+MVg+PW1a4Ox1rH+h14dqUApG1Yyzt52HUvbFYW17IHB1KGLzmsIOx/LwGC7BE4CJ60jYnJq36unw/OTka6LpQpOYNpptZP/WvXru6jBlqCdjAjpl3EatnL7yow9w9h657nhJ7N03gynXeZMCZwETuiImJGI7+bkvptYQVJwklr6o+tO/XeXWndSlJHGJ7ES7bRdU3XablBRK3JFGAasPO84bOWuta87CZw2dbuTwfuQ9V6ctNN2o36SCVu2K0KH1XkdUxqcdlmrJnOcPhQ4CZzii5O5Zy9rxcbe9rgNqnw+Sj9pK1Fm2snU8rPSTh/KHx8KnARO8cMpHtppu9EPEQ9jT+d8OG/YZO2K2GVXd/pQGHsCpzdIO2nGUt4uf1+msXfeUGE6r3Xt6XBSzb1dyxvy/0OBk8ApcbTTe5b1p2VrJ32N6bzRGWHrKN8lXBECpzdYO203NuXqiFrp/E7njRWnWCak2SVwEji96drJxNh7bwXGXpSv/Lz5DBoWpp5lu9OHAieBU+LXnbabtuaufPZBDVbRPcp3WXfYM8PpQ/3KhwIngVNiaaft+obcuDjKNbrpvNbgszT2LHzmwtgTOL3Jnr1oa29lzbgmxp5Fu9P7ZpafwEng9KbWneI5N+55o0PvvGW70y4LU2+XcJQLnN5sz972+M7cfj7as2cZ77TLeapp0YwrcHqzPHvxmmpaH5Xh2O60ywIqC+30YTRdAieBU2J79uJl7J2P+m/f7rRL1J0EThvBs6f3RCx35vbzUcaesQVKj5MdVU44iS6wAqeE9ezF21Fu1QJlr51sjb0PhXYSOL0Jdaft78XR2DPRTefNPXu7DCbeLhHcLnBaR+30XjxGMoqvK8JJrF0RYugVgdNa4eQsMk7OstRzrgpO8U/5YQyy1Iv/xVlknJyFF9cYJOaUZPVSChEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIgQIUKECBEiRIiT/HuQ/5PJPzP5n7L8gct/APmvIP+qyN/J8n+A/BuQf4vyH7n80z/909/+7d/+8Y9//N9A/uZv/vSnP+GwlP/pH/5h+3Y6rmtWVta77771u9/RURPZKIt0ELn333+fjVLMRRnW8f/RyX9n8u+o/O8o/wXl/xLvUkgC4/SH/2mB09/h35ripAHqv+OfQpPASci6inf+xnH4nBsbWyzX4fTPCk7/rNBEgfoPf5Bx+q8MJsbTvy4Bpz9Z4fS2jNPbCk4f4h/CpNNOfy/DZOAJYYoTTsacESLESQIv72Chqb1x3NtwQrLRTn+w1E4a5UR5Wpp22m6mnRhNu2LUTqtj7EXljJCYpHYxjxD/sQ7l+7gh8wYgQRopljcP7C71vr6LX4q1KWv6+/untd8n83Rn0XzHpIPaXTMrfojw6+rlHTcVxELTeU4itaN5dtpJAUqvnf7uX+OpnVT15KCdVJpk9RRv7RSVM0Jiw2lsmnjbyqxxwgK/KMns1FZ5zlzxePCbHqcZKXDteExXhKRBLWwrx6mlsm+YmygvqjxliHVNlcfjOaO7oYGmZjlJ37B860H2G1xNOvU4rY920lad7LTT3xvrTubaSZMJ3gZY9eBrDryE579LlpozQmLD6fmdjprnVzpq7txpPQ4qvuncyLM7kIkk8Kw7UNHsffl4ceRZ6PnNvjvAHSFtHiqYw8V9d3qHnxWSznbGCCigwIv+ydLa/otPh4PAzLX+yfLayYv9Fy/2d8B3ul2fFD76pwEnfty15emY4ipFL3aGpvNfhJqxJA3n5+/T8O6dKwoV4kpb2XD+S0hSPFYEVkxQriHcOSfZaieZp9WsO+mtPWftpCinf2eunbSZ8CQ//3XTNHJ15u4XL0PdS80ZIbHhND6/+LL5WQdmdHPnCal2HD6K0VzuHKq9Mx6cBGMPtRN+AkPBHqQphFjQTXPj4Zf4amru9N8ZJsXTpGW6FkiaAXxg64tu+FI8Q+YLESfcLjFjr5olhY/aGcCJH7e8J/D3DCkl4yS8en8T8F3T262vWTf0Pa4slFMHKuQiQgsN3d9O1l07ydMR7YpT3UmfCYEKNCeCle2YCaplEWPOCIkRp/Cz8cCzjmB/f29zWyF8b+i7c2cIi/3zF8NXnk7XMJzGpSDiRMIvPJ7WUsLqTv4b+VcK6GY09p52zz2/dm0YsPB//mpG8oNWApxI7TQpHqY4wfY8TBoEs5AmnWtmOMnHLUs6WyNq0WgtZ4VILkk1lVBwaqsKSVekhhaa2io0bNpay/WFZv6GvWdvbepOlKhdcfPs6XDyNoxG5Of3NpzNW2LOCIkRJ2kkAjg1FHpfdncOASSd/Mc+/Gwxb66v24ATIXOLrPjCptrFvLY707xCFH7RXYzrMk5zzd4X5jhJ86CzMOk8aCXASeLHebcsp9Jc8fxKUdmMxDXVmcfHTrC6U4h6eDtDhfy3mBWaYlpN7CxjNYqTRZ4QJB+40lpN1l87vbMc7WRfdwopbu7iolDfIG7DXACclpgzQmLFCetJHfN3+q80+6887x+HutNz+qsGlaIgtfH8x55/o+KkVGB779zoln8Ba6709w9LUAe6Vi3j1NJ/8ZoFTuEXgzSp/2l//4z/6Qw/rm18GVa6vwlM/rkq/hvQUuU5g25D774vblZiDS988szL1uPEUGiKVd8LStcUv7Bd3Wn1251kz96S604W2knJBJS9+754VtYN1hzwMdB0VlpizghZE6lZzLNw38WI8/L9ejWV6BMJYlnwnmSlpnisOfCyjJs4xbTCHWwKNRNi/hscJYnh2Xt7KZ49h3anYo3XgdaOgsc8nrIq1OBLyhkha0LTnUHTVsAXwzE1Fn6DXonlijc/P7+eUJy4yR+oOCFXuamtg6VloNIzpCk0hhqCFU7rWHeKb7sTywTZLqYtsuGP/U2FS80ZIZtD/D1QRrwnz+bR9XbUVBwn+nMbqDjXxtRVDfdfQfJwhYXzNyE8e7viVXciBuONevWIzMzSckbIJpE2bGsqKiTBK9Pek2fu5s/BOunK33cTXVfehjPHAxVgCYbzX1dN50d48lAzWZp2+sNatju9vVTPnnm7k1vOBMgZEizY97qHa555dEcsMWeEbBLxzlV5yoYl+I09IflfFtGGfewEUDaTh66JQvz1HZKKafNzO3r6se2fkCVppzcyQEPJBMyZOfTyYbXI+/pKCJu9l5gzQoQIMfn1eTFZKnJBiBAhQoQIESJEiBAhQoQIESJEiBAhQoQIESJEiBAhQoQI2dBSXHQujy1qq8alDf2AolerkNUvbdjdM1DhOTfQdELa0A8ocBKy+qXNczYPPzdqadvwDygkoUrbWKgwUNFHjb3iUH+lZzGyQR+w5kqRp6+7zTOe0eApFG9eyKqUtudVo3PwQXEqKpvs2WBFTX3A4JX+K55z/p6yx1VnxRiUQlantA01eMZaX3Ochkinp32DPqCEI9SM5nV6PKFu8eKFrFJpq6n0tNcqOBVvPJz4A3a9HPNAPcpf6REDJAtZtdJG2kbzNjRO/AEbQtOvKs9KbZ6xkKg6CVm10uadIBsbJ/aAJz2TLz1nayrB8BMDFQlZtdJGyAbHiT3gQJPnecXos1Cht8EzJN68ECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRIkSIECFChAgRsjHk/wc8a+q7GUqa2gAAAABJRU5ErkJggg==\">\n      </div>\n      <div class=\"modal-footer\">\n        <button type=\"button\" class=\"btn btn-default\" data-dismiss=\"modal\" style=\"font-size:larger;\">Close</button>\n      </div>\n    </div>\n  </div>\n</div>\n\n<button type=\"button\" class=\"btn btn-default\" data-toggle=\"modal\" data-target=\"#modal-credits\" style=\"font-size:larger;\">Credits</button>\n<div class=\"modal fade\" id=\"modal-credits\" tabindex=\"-1\" role=\"dialog\" aria-labelledby=\"modal-credits\">\n  <div class=\"modal-dialog\" role=\"document\">\n    <div class=\"modal-content\">\n      <div class=\"modal-header\">\n        <button type=\"button\" class=\"close\" data-dismiss=\"modal\" aria-label=\"Close\"><span aria-hidden=\"true\">×</span></button>\n        <h1 class=\"modal-title\" id=\"modal-credits-label\">Credits</h1>\n        <hr>\n      </div>\n      <div class=\"modal-body modal-credits-body\">\n        <h2>Atomic Data:</h2>\n\n        <p>This notebook is based on the NOMAD Atomic Data Parser and Interface written by <a href=\"mailto:regler@fhi-berlin.mpg.de\">Benjamin Regler</a>.</p>\n        <ul>\n          <li><span class=\"authors\">Regler, B.</span>: <em>NOMAD Atomic Data Parser and Interface</em>. Fritz Haber Institute of the Max Planck Society, Germany (2017).</li>\n        </ul>\n\n        <h2>Atomic Data Collections:</h2>\n        <dl>\n          <dt>Experimental and theoretically derived values for isotropic static polarizability</dt>\n          <dd>\n            <p>This collection includes experimental and theoretically derived values for isotropic static polarizability as complied by <a href=\"http://ctcp.massey.ac.nz/?group=schwerd\">Prof. Peter Schwerdtfeger</a>.</p>\n            <ul>\n              <li><span class=\"authors\">Schwerdtfeger, P.</span>: <em>Table of experimental and calculated static dipole polarizabilities for the electronic ground states of the neutral elements (in atomic units)</em>. Centre for Theoretical Chemistry and Physics, The New Zealand Institute for Advanced Study (2014). [<a href=\"http://ctcp.massey.ac.nz/Tablepol2014.pdf\">link</a>]</li>\n            </ul>\n            <p>Not all published values are compiled, only the most accurate ones. There is some confusion about the experimental data listed in the <a href=\"https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286\">CRC Handbook of Chemistry and Physics</a> taken from Miller and Bederson. Some of the data are not experimental values as indicated, but from LDA calculations of Doolen, which are listed here as well.</p>\n            <p>A more recent review by Mitroy, Safronova and Clark is highly recommended:</p>\n            <ul>\n              <li><span class=\"authors\">Mitroy, J.; Safronova, M. S. &amp; Clark, C. W</span>: <em>Theory and applications of atomic and ionic polarizabilities</em>. Journal of Physics B: Atomic, Molecular and Optical Physics <strong>43</strong>, 202001 (2010). DOI: <a href=\"https://dx.doi.org/10.1088/0953-4075/43/20/202001\">10.1088/0953-4075/43/20/202001</a>.</li>\n            </ul>\n          </dd>\n\n          <dt>Experimental electron affinities for neutral atoms</dt>\n          <dd>\n            <p>The values for experimental electron affinity for neutral atoms are taken from</p>\n            <ul>\n              <li><span class=\"authors\">Lide, D. R.</span>: <em>CRC Handbook of Chemistry and Physics 86th ed.</em>. CRC Press, 2616 pp. (2005). [<a href=\"https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286\">link</a>]</li>\n            </ul>\n          </dd>\n\n          <dt>Extended binaries, dimers and atoms</dt>\n          <dd>\n            <p>This collection provides data for extended binaries, dimers, and atoms. It contains atom property information for rock-salt and zincblende crystal lattice structures, octet (I/II/III)-(V/VI/VII) binary materials, other eight-electron binaries using possible valences of d-metals and f-elements, and octet binaries from John and Bloch's paper:</p>\n            <ul>\n              <li><span class=\"authors\">John, J. &amp; Bloch, A. N.</span>: <em>Quantum-Defect Electronegativity Scale for Nontransition Elements</em>. Physical Review Letters, American Physical Society, <strong>33</strong>, 1095-1098 (1974). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.33.1095\">10.1103/PhysRevLett.33.1095</a>.</li>\n            </ul>\n            <p>The atomic properties in this collection are obtained from:</p>\n            <ul>\n              <li><span class=\"authors\">Ghiringhelli, L. M.; Vybiral, J.; Levchenko, S. V.; Draxl, C. &amp; Scheffler</span>: <em>M. Big Data of Materials Science: Critical Role of the Descriptor</em>. Physical Review Letters, American Physical Society <strong>114</strong>, 105503 (2015). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.114.105503\">10.1103/PhysRevLett.114.105503</a>.</li>\n            </ul>\n          </dd>\n        \n          <dt>Isotropic static polarizabilities and homo-atomic van der Waals coefficients for neutral free atoms</dt>\n          <dd>\n            <p>The majority of values such as isotropic static polarizability (in bohr<sup>3</sup>) and the homo-atomic van der Waals coefficient (in hartree · bohr<sup>6</sup>) for neutral free atoms are taken from:</p>\n            <ul>\n              <li><span class=\"authors\">Chu, X. &amp; Dalgarno, A.</span>: <em>Linear response time-dependent density functional theory for van der Waals coefficients</em>. The Journal of Chemical Physics <strong>121</strong>, 9, 4083 (2004). DOI: <a href=\"https://dx.doi.org/10.1063/1.1779576\">10.1063/1.1779576</a>.</li>\n              \n              <li><span class=\"authors\">Mitroy, J.; Safronova, M. S. &amp; Clark, C. W</span>: <em>Theory and applications of atomic and ionic polarizabilities</em>. Journal of Physics B: Atomic, Molecular and Optical Physics <strong>43</strong>, 202001 (2010). DOI: <a href=\"https://dx.doi.org/10.1088/0953-4075/43/20/202001\">10.1088/0953-4075/43/20/202001</a>.</li>\n            </ul>\n            <p>The rest of the elements are calculated using linear response coupled cluster single double theory with accurate basis. The van der Waals radii for the respective elements are defined as discussed in:</p>\n            <ul>\n              <li><span class=\"authors\">Tkatchenko, A. &amp; Scheffler</span>: <em>Accurate Molecular Van Der Waals Interactions from Ground-State Electron Density and Free-Atom Reference Data</em>. Physical Review Letters <strong>102</strong>, 073005 (2009). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevLett.102.073005\">10.1103/PhysRevLett.102.073005</a>.</li>\n            </ul>\n            <p>For lanthanides and actinides, the C<sub>6</sub> coefficients are constructed to satisfy the valence electronic sum rule using the one-term formula which is equivalent to the two-point zeroth-order Padé approximant. Here, static polarizabilities are taken from:</p>\n            <ul>\n              <li><span class=\"authors\">Dzuba, V. A.; Kozlov, A.; Flambaum; V. V.</span>: <em>Scalar Static Polarizabilities of Lanthanides and Actinides</em>. Physical Review A <strong>89</strong>, 042507 (2014). DOI: <a href=\"https://dx.doi.org/10.1103/PhysRevA.89.042507\">10.1103/PhysRevA.89.042507</a>.</li>\n            </ul>\n          </dd>\n        </dl>\n      </div>\n      <div class=\"modal-footer\">\n        <button type=\"button\" class=\"btn btn-default\" data-dismiss=\"modal\" style=\"font-size:larger;\">Close</button>\n      </div>\n    </div>\n  </div>\n</div>\n\n<p></p>"
+                },
+                "selectedType": "BeakerDisplay",
+                "elapsedTime": 0,
+                "height": 100
+            },
+            "evaluatorReader": true,
+            "lineCount": 126
+        },
+        {
+            "id": "markdownaIbvLV",
+            "type": "markdown",
+            "body": [
+                "### Atomic data collection viewer",
+                "",
+                "The atomic data collection viewer provides an interface to display atomic data collections in the periodic table elements.  The elements will be colored by the value of the selected atomic property. Elements that are not listed in the atomic collections are shown in gray and more detailed information about an element can be found by moving the mouse over an element.",
+                "",
+                "#### Atomic data collections",
+                "",
+                "The visualization of the periodic table of elements is based on the selected atomic data collections. The available atomic data collections are listed in the following box. Please select one or more atomic data collections for the visualization.",
+                "",
+                "<div class=\"atomic-data row\">",
+                " <div class=\"atomic-data--block atomic-data--collection col-lg-11 col-md-10\">",
+                "  <label for=\"atomic-data--select-collection\">Atomic data collections:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-collection\" data-placeholder=\"Nothing selected\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                " ",
+                " <div class=\"atomic-data--block atomic-data--collection col-lg-1 col-md-2\">",
+                "  <button type=\"button\" class=\"atomic-data--reset-buton btn btn-danger\" id=\"atomic-data--reset-collection\" title=\"Reset atomic data collection selection\">Reset</button>",
+                " </div>",
+                "</div>",
+                "<p>You have selected <span id=\"atomic-data--collection-counter\">0</span> atomic data collection(s).</p>",
+                "",
+                "<h4>Filters</h4>",
+                "",
+                "You can use filters to select only a specific subset of atomic data collections. Filters that are not available are disabled.",
+                "",
+                "<div class=\"atomic-data row\">",
+                " <div class=\"atomic-data--block atomic-data--filters col-lg-2 col-md-3\">",
+                "  <label for=\"atomic-data--select-source\">Source:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-source\" data-placeholder=\"Nothing selected\" data-name=\"source\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                "  ",
+                " <div class=\"atomic-data--block atomic-data--filters col-lg-2 col-md-4\">",
+                "  <label for=\"atomic-data--select-method\">Method:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-method\" data-placeholder=\"Nothing selected\" data-name=\"method\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                "",
+                " <div class=\"atomic-data--block atomic-data--filters col-lg-3 col-md-5\">",
+                "  <label for=\"atomic-data--select-basis_set\">Basis set:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-basis_set\" data-placeholder=\"Nothing selected\" data-name=\"basis_set\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                "",
+                " <div class=\"atomic-data--block atomic-data--filters col-lg-3 col-md-7\">",
+                "  <label for=\"atomic-data--select-doi\">References:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-doi\" data-placeholder=\"Nothing selected\" data-name=\"doi\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                "",
+                " <div class=\"atomic-data--block atomic-data--filters col-lg-2 col-md-5\">",
+                "  <label for=\"atomic-data--select-term_symbol\">Term symbols:</label>",
+                "  <select class=\"atomic-data--select chosen-select\" id=\"atomic-data--select-term_symbol\" data-placeholder=\"Nothing selected\" data-name=\"term_symbol\" multiple=\"multiple\" disabled=\"disabled\" size=\"6\"></select>",
+                " </div>",
+                "</div>",
+                "",
+                "#### Atomic properties",
+                "",
+                "Please select the atomic property to be visualized in the periodic table of elements. The elements will be colored by the value of the selected atomic property. A colormap shows the range of the atomic property value (including the minimum and maximum value). Leaving this field empty means displaying all available atomic properties in the table without a colormap.",
+                "",
+                "<div class=\"atomic-data row\">",
+                " <div class=\"atomic-data--block atomic-data--properies col-md-4\">",
+                "  <label for=\"atomic-data--select-properties\">Atomic properties:</label>",
+                "  <select class=\"atomic-data--select chosen-select-deselect\" id=\"atomic-data--select-properties\" data-placeholder=\"Nothing selected\" disabled=\"disabled\">",
+                "   <option value=\"\"></option>",
+                "  </select>",
+                " </div>",
+                " ",
+                " <div class=\"atomic-data--block atomic-data--properties col-lg-1 col-md-2\">",
+                "  <button type=\"button\" class=\"atomic-data--reset-buton btn btn-danger\" id=\"atomic-data--reset-properties\" title=\"Reset atomic property selection\">Reset</button>",
+                " </div>",
+                "</div>",
+                "",
+                "#### Visualization",
+                "",
+                "<div class=\"periodic-table\"></div>",
+                "",
+                "<h3 style=\"margin-top: 0;\">Feedback</h3>",
+                "<p>Want to give feedback?<br /><br />",
+                " <a target=\"_blank\" href=\"https://nomad-forum.rz-berlin.mpg.de\" class=\"btn btn-primary\" style=\"font-size: larger\">Send your feedback to the Analytics Toolkit Forum</a>",
+                "</p>",
+                "<p>Your comments are invaluable in helping us to provide a user-friendly experience for all!<p>"
+            ],
+            "evaluatorReader": false
+        },
+        {
+            "id": "setup_notebook",
+            "type": "code",
+            "evaluator": "JavaScript",
+            "input": {
+                "body": [
+                    "/*",
+                    "  Small javascript library to generate a color palette.",
+                    "",
+                    "  @namespace jPalette",
+                    "  @version 0.4.0",
+                    "  @author Julien Descamps",
+                    " */",
+                    "!function(e){\"use strict\";var n=function(e,n,t,r){this.r=e||0,this.g=n||0,this.b=t||0,this.a=r||0};n.prototype.delta=function(e){return new n(this.r-e.r,this.g-e.g,this.b-e.b,this.a-e.a)},n.prototype.rgb=function(){return\"rgb(\"+this.r+\",\"+this.g+\",\"+this.b+\")\"},n.get=function(e){return function(t){switch(e){default:case\"white\":return new n(255,255,255,t);case\"black\":return new n(0,0,0,t);case\"red\":return new n(255,0,0,t);case\"green\":return new n(0,255,0,t);case\"blue\":return new n(0,0,255,t);case\"yellow\":return new n(255,255,0,t);case\"cyan\":return new n(0,255,255,t);case\"magenta\":return new n(255,0,255,t);case\"indigo\":return new n(128,0,255,t);case\"pink\":return new n(255,0,128,t);case\"orange\":return new n(255,128,0,t);case\"apple\":return new n(128,255,0,t);case\"manganese\":return new n(0,128,255,t);case\"guppie\":return new n(0,255,128,t);case\"purple\":return new n(128,0,128,t);case\"teal\":return new n(0,128,128,t);case\"olive\":return new n(128,128,0,t);case\"coral\":return new n(255,128,128,t)}}};var t=function(e,n){if(n.length<=1)throw\"Two colors minimum.\";this.map=[],this.numSteps=e,this.colors=n,this.init()};t.prototype.init=function(){var e,t,r,s,w,a,i=1/(this.colors.length-1),o=this,u=function(e){return parseInt(o.colors[r][e]+w*a[e],10)};for(e=0;e<this.numSteps;e++)t=e/(this.numSteps-1),r=Math.floor(t/i),s=Math.min(this.colors.length-1,r+1),w=(t-r*i)/i,a=this.colors[s].delta(this.colors[r]),this.map.push(new n(u(\"r\"),u(\"g\"),u(\"b\"),u(\"a\")))},t.prototype.getColor=function(e){var n=Math.max(0,Math.min(1,e)),t=Math.floor(n*(this.map.length-1));return this.map[t]},t.get=function(e){return function(r){switch(e){default:case\"whitetoblack\":return new t(r,[new n(255,255,255,255),new n(0,0,0,255)]);case\"rgb\":return new t(r,[new n(255,0,0,255),new n(0,255,0,255),new n(0,0,255,255)]);case\"rainbow\":return new t(r,[new n(255,0,0,255),new n(255,128,0,255),new n(255,255,0,255),new n(0,255,0,255),new n(128,0,128,255),new n(128,0,255,255)]);case\"night\":return new t(r,[new n(0,0,102,255),new n(255,255,255,255),new n(255,102,0,255),new n(0,0,102,255)]);case\"blacknwhite\":return new t(r,[new n(255,255,255,255),new n(0,0,0,255),new n(255,255,255,255),new n(0,0,0,255)]);case\"fire\":return new t(r,[new n(0,0,0,255),new n(255,0,0,255),new n(255,255,0,255),new n(255,0,0,255)]);case\"sky\":return new t(r,[new n(0,0,120,255),new n(200,255,255,255),new n(0,0,120,255)])}}},e.Color=n,e.ColorMap=t}(window.jPalette=window.jPalette||{});",
+                    "/*",
+                    " Periodic Table",
+                    "",
+                    " @copyright Copyright 2017 Benjamin Regler - MIT License",
+                    " @license   https://opensource.org/licenses/MIT",
+                    " @author    Benjamin Regler",
+                    " @version   1.0.0",
+                    "*/",
+                    "Object.extend=function(e,n){for(var a in n)n.hasOwnProperty(a)&&!e.hasOwnProperty(a)&&(e[a]=n[a]);return e},$.fn.contrastColor=function(){return this.each(function(){var e=$(this).css(\"background-color\");if((\"transparent\"==e||\"rgba(0, 0, 0, 0)\"==e)&&($(this).parents().each(function(){return e=$(this).css(\"background-color\"),\"transparent\"!=e&&\"rgba(0, 0, 0, 0)\"!=e?!1:void 0}),\"transparent\"==e||\"rgba(0, 0, 0, 0)\"==e))return!1;var n=e.replace(/^(rgb|rgba)\\(/,\"\").replace(/\\)$/,\"\").replace(/\\s/g,\"\").split(\",\"),a=(299*n[0]+587*n[1]+114*n[2])/1e3;a>=128?$(this).removeClass(\"light-color\"):$(this).addClass(\"light-color\")})},String.prototype.capitalize=function(){return this.charAt(0).toUpperCase()+this.slice(1)},function(e){\"use strict\";var n=function(e){var n={minpos:0,maxpos:100,minval:0,maxval:1,scale:.01},a=function(e,n){for(var a in n)n.hasOwnProperty(a)&&e[a](n[a]);return e},t=function(){n.scale=(n.maxval-n.minval)/(n.maxpos-n.minpos)},i=function(){return n.scale},o=function(e){return\"undefined\"!=typeof e&&(n.minpos=e,t()),n.minpos},r=function(e){return\"undefined\"!=typeof e&&(n.maxpos=e,t()),n.maxpos},l=function(e){return\"undefined\"!=typeof e&&(n.minval=e,t()),n.minval},s=function(e){return\"undefined\"!=typeof e&&(n.maxval=e,t()),n.maxval},c={scale:i,minpos:o,maxpos:r,minval:l,maxval:s};return a(c,e||{})},a=function(e){var a=function(e){var n=this.minval(),a=this.scale()*(e-this.minpos())+n;return Math.min(Math.max(a,n),this.maxval())},t=function(e){var n=this.minpos(),e=(e-this.minval())/this.scale()+n;return Math.min(Math.max(e,n),this.maxpos())},i=new n(e),o={value:a,position:t};return Object.extend(o,i)},t=function(e){e.minval=\"undefined\"!=typeof e.minval?e.minval:1,e.maxval=\"undefined\"!=typeof e.maxval?e.maxval:1e3;var a=function(e){var n=Math.log(this.minval()),a=Math.exp(this.scale()*(e-this.minpos())+n);return Math.min(Math.max(a,this.minval()),this.maxval())},t=function(e){var n=Math.log(this.minval()),e=this.minpos()+(Math.log(e)-n)/this.scale();return Math.min(Math.max(e,this.minpos()),this.maxpos())},i=function(){var e=Math.log(this.minval()),n=Math.log(this.maxval());return(n-e)/(this.maxpos()-this.minpos())},o=new n(e),r={value:a,position:t,scale:i};return Object.extend(r,o)},i=function(e,n){return{name:e,colors:n||[],map:new jPalette.ColorMap(500,n)}},o=function(e){var n,o={enabled:!0,scale:\"linear\",min:0,max:100,value:0,colormap:new i(\"thermometer\",[new jPalette.Color(0,0,255,255),new jPalette.Color(255,0,0,255)])},r=function(e){if(!n||\"undefined\"!=typeof e){var i={minpos:o.min,maxpos:o.max,minval:1,maxval:2};switch(o.type){case\"logarithmic\":e=new t(i);break;case\"linear\":default:e=new a(i)}n=e}return n},l=function(e,n){r();for(var a in n)n.hasOwnProperty(a)&&e[a](n[a]);return e},s=function(e){return\"undefined\"!=typeof e&&(o.enabled=!!e),o.enabled},c=function(e){return\"undefined\"!=typeof e&&(e=e.constructor===Array?new i(\"custom\",e):\"thermometer\"==e?new i(\"thermometer\",[new jPalette.Color(0,0,255,255),new jPalette.Color(255,0,0,255)]):new i(e,jPalette.ColorMap.get(e)(0).colors),o.colormap=e),o.colormap},u=function(e){return\"undefined\"!=typeof e&&([\"linear\",\"logarithmic\"].indexOf(e)<0?console.log(\"[error] Colormap scale is not supported. 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+                    "/*!",
+                    " Atomic Data",
+                    "",
+                    " @copyright  Copyright 2017 Fritz Haber Institute of the Max Planck Society,",
+                    "             Benjamin Regler - Apache 2.0 License",
+                    " @license    http://www.apache.org/licenses/LICENSE-2.0",
+                    " @author     Benjamin Regler",
+                    " @version    1.0.0",
+                    " ",
+                    " Licensed under the Apache License, Version 2.0 (the \"License\");",
+                    " you may not use this file except in compliance with the License.",
+                    " You may obtain a copy of the License at",
+                    " ",
+                    "     http://www.apache.org/licenses/LICENSE-2.0",
+                    "",
+                    " Unless required by applicable law or agreed to in writing, software",
+                    " distributed under the License is distributed on an \"AS IS\" BASIS,",
+                    " WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.",
+                    " See the License for the specific language governing permissions and",
+                    " limitations under the License.",
+                    " */",
+                    "!function(e){\"use strict\";var t=function(e){var t=(window.beaker||{},null),n={search_contains:!0,width:\"100%\",allow_single_deselect:!0},a={connector:null,namespace:e.namespace||\"\",id:null,collections:[],collection:{},elements:{},atomic_properties:{}},o=function(e){var t,n=0;for(t in e)e.hasOwnProperty(t)&&n++;return n},r=function(e,t){try{var n=e.toString(),a=n.indexOf(\".\"),o=n.indexOf(\"e\"),t=t||2,r=parseFloat(e);return isNaN(r)?e:(o>0?(n=r.toPrecision(t)+\"\",n=n.replace(\"e\",\"x10<sup>\")+\"</sup>\"):a>0&&(a>t?(n=r.toExponential(t)+\"\",n=n.replace(\"e\",\"x10<sup>\")+\"</sup>\"):a+t<n.length&&(n=r.toFixed(t)+\"\")),n.replace(/\\.?0+(?:(?=x)|$)/,\"\")||\"0\")}catch(i){return e}},i=function(e,t){var n=a.connector,o=n.variable(e)||[];if(\"undefined\"==typeof t)o=[];else if(t.selected&&$.inArray(t.selected,-1==o))o.push(t.selected);else{var r=$.inArray(t.deselected,o);t.deselected&&r>=0&&o.splice(r,1)}return n.variable(e,o),o},c=function(n){var 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+                ],
+                "hidden": true
+            },
+            "output": {
+                "hidden": true,
+                "state": {},
+                "pluginName": "JavaScript",
+                "selectedType": "Text"
+            },
+            "evaluatorReader": true,
+            "lineCount": 39,
+            "initialization": true
+        },
+        {
+            "id": "atomic_data",
+            "type": "code",
+            "evaluator": "IPython",
+            "input": {
+                "body": [
+                    "#!/usr/bin/python",
+                    "# -*- coding: utf-8 -*-",
+                    "\"\"\"",
+                    "@package    atomic_data",
+                    "@copyright  Copyright 2017 Fritz Haber Institute of the Max Planck Society,",
+                    "            Benjamin Regler - Apache 2.0 License",
+                    "@license    http://www.apache.org/licenses/LICENSE-2.0",
+                    "@author     Benjamin Regler",
+                    "@version    1.0.0",
+                    "",
+                    "Licensed under the Apache License, Version 2.0 (the \"License\");",
+                    "you may not use this file except in compliance with the License.",
+                    "You may obtain a copy of the License at",
+                    "",
+                    "    http://www.apache.org/licenses/LICENSE-2.0",
+                    "",
+                    "Unless required by applicable law or agreed to in writing, software",
+                    "distributed under the License is distributed on an \"AS IS\" BASIS,",
+                    "WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.",
+                    "See the License for the specific language governing permissions and",
+                    "limitations under the License.",
+                    "\"\"\"",
+                    "",
+                    "import os",
+                    "import re",
+                    "import json",
+                    "",
+                    "from atomic_data import common",
+                    "from atomic_data.collections import AtomicCollection",
+                    "",
+                    "",
+                    "class AtomicDataController:",
+                    "    \"\"\"Atomic Data Controller",
+                    "    \"\"\"",
+                    "",
+                    "    # Cache to speed things up",
+                    "    _cache = {}",
+                    "",
+                    "    # Beaker instance",
+                    "    _beaker = None",
+                    "",
+                    "    # Python event queue",
+                    "    _events = []",
+                    "",
+                    "    def __init__(self):",
+                    "        # Get Beaker instance",
+                    "        if beaker is not None:",
+                    "            self._beaker = beaker",
+                    "",
+                    "    def execute(self):",
+                    "        # Read Atomic Data Beaker event queue",
+                    "        try:",
+                    "            events = self._beaker.get('atomic_data_events')",
+                    "        except:",
+                    "            # Nothing to do",
+                    "            return",
+                    "",
+                    "        # Execute events",
+                    "        self._events = []",
+                    "        for data in events:",
+                    "            event, params = data",
+                    "",
+                    "            # Make sure parameters are always passed as a list",
+                    "            if not isinstance(params, (tuple, list)):",
+                    "                params = [params]",
+                    "",
+                    "            method = getattr(self, self._get_event(event), None)",
+                    "            if callable(method):",
+                    "                data = method(*params)",
+                    "",
+                    "                # Add data to Atomic Data Beaker event queue",
+                    "                if data is not None:",
+                    "                    _, event = event.split('_', 1)",
+                    "                    self.add_event(event, data)",
+                    "",
+                    "        # Ignore events that have not been found",
+                    "        self._beaker.set('atomic_data_events', self._events)",
+                    "        self._events = []",
+                    "",
+                    "    def add_event(self, name, arguments):",
+                    "        # Make sure parameters are always passed as a list",
+                    "        if not isinstance(arguments, (tuple, list)):",
+                    "            arguments = [arguments]",
+                    "",
+                    "        self._events.append([name, arguments])",
+                    "",
+                    "    def get_collections(self, path):",
+                    "        collections = self._cache.get('collections', [])",
+                    "        if not collections:",
+                    "            # Resolve path",
+                    "            path = os.path.expanduser(os.path.normpath(path))",
+                    "",
+                    "            # List all available collections",
+                    "            for filename in os.listdir(path):",
+                    "                filepath = os.path.join(path, filename)",
+                    "                collection = common.get_collection(filepath)",
+                    "                collections.append({",
+                    "                    'path': filepath,",
+                    "                    'filename': filename,",
+                    "                    'title': collection.get_title(),",
+                    "                    'description': collection.get_description()",
+                    "                })",
+                    "",
+                    "            # Sort collection based on titles (in-place)",
+                    "            collections.sort(key=lambda c: c['title'])",
+                    "            self._cache['collections'] = collections",
+                    "",
+                    "        # Return collections",
+                    "        return [collections]",
+                    "",
+                    "    def get_elements(self, path):",
+                    "        # Resolve path",
+                    "        path = os.path.expanduser(os.path.normpath(path))",
+                    "        filename = os.path.join(path, 'periodic_table.min.json')",
+                    "",
+                    "        # Get elements",
+                    "        elements = {}",
+                    "        if not elements:",
+                    "            with open(filename) as file:",
+                    "                elements = json.load(file)",
+                    "",
+                    "        # Return elements",
+                    "        return elements",
+                    "",
+                    "    def get_collection(self, collections):",
+                    "        # Create atomic data collection",
+                    "        c = AtomicCollection('beaker-collection', collections=collections)",
+                    "",
+                    "        # Get all available atomic methods and their possible options",
+                    "        methods = dict.fromkeys(c.get_atomic_methods(), [])",
+                    "        for method in methods:",
+                    "            methods[method] = list(sorted(c.get_atomic_methods(method)))",
+                    "",
+                    "        # Pack atomic properties and options into a dictionary",
+                    "        data = {",
+                    "            'methods': methods,",
+                    "            'properties': list(sorted(c.get_atomic_properties()))",
+                    "        }",
+                    "",
+                    "        # Add collection information to Atomic Data Beaker event queue",
+                    "        self.add_event('collection', data)",
+                    "",
+                    "        # Store current collection for later use",
+                    "        self._cache['collection'] = {",
+                    "            'hash': hash(','.join(collections)),",
+                    "            'instance': c",
+                    "        }",
+                    "",
+                    "        # Return data",
+                    "        return data",
+                    "",
+                    "    def get_atomic_properties(self, collections, filters={}):",
+                    "        collection = self._cache.get('collection', None)",
+                    "        if collection:",
+                    "            # Check hash",
+                    "            chash = hash(','.join(collections))",
+                    "            if chash == collection['hash']:",
+                    "                collection = collection['instance']",
+                    "                collections = []",
+                    "",
+                    "        # Get collection",
+                    "        if collections:",
+                    "            collection = self.get_collection(collections)",
+                    "",
+                    "        # Get all atomic properties",
+                    "        properties = {}",
+                    "        for prop in collection.get_atomic_properties():",
+                    "            # Remove empty values in filter dictionary",
+                    "            filters = dict((k, v) for k, v in filters.items() if v)",
+                    "            ",
+                    "            # Set default source, if None is available",
+                    "            if 'source' not in filters:",
+                    "                source = collection.get_atomic_methods('source')",
+                    "                if len(source) > 0:",
+                    "                    filters['source'] = list(source)",
+                    "",
+                    "            # Apply filters on atomic property",
+                    "            p = collection.get(prop, **filters)",
+                    "",
+                    "            # Index data based on atomic number, not on atomic symbol",
+                    "            data = {}",
+                    "            for symbol, item in p.data():",
+                    "                item = {k: (list(v) if isinstance(v, set) else v)",
+                    "                        for k, v in item.items()}",
+                    "                data[item['index']] = item",
+                    "            properties[prop] = data",
+                    "",
+                    "        # Return atomic properties",
+                    "        return properties",
+                    "",
+                    "    def _get_event(self, name):",
+                    "        return re.sub('(?<!^)(?=[A-Z])', '_', name).lower().lstrip('_')",
+                    "",
+                    "",
+                    "# Main cycle",
+                    "if __name__ == '__main__':",
+                    "    controller = AtomicDataController()"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "hidden": true,
+                "state": {},
+                "pluginName": "IPython",
+                "shellId": "D6AB0868E05747479E7342FBBCD277FD"
+            },
+            "evaluatorReader": true,
+            "lineCount": 197,
+            "initialization": true
+        },
+        {
+            "id": "init_notebook",
+            "type": "code",
+            "evaluator": "JavaScript",
+            "input": {
+                "body": [
+                    "/**",
+                    " * Initialization",
+                    " */",
+                    ";(function() {",
+                    "    // Set module namespace",
+                    "    if (typeof window.AtomicData == \"undefined\") {",
+                    "        window.AtomicData = {};",
+                    "    }",
+                    "    var namespace = window.AtomicData;",
+                    "",
+                    "    /**",
+                    "     * Properties",
+                    "     */",
+                    "    var instances = {},",
+                    "        connector = {",
+                    "            \"evaluator\": \"connector\",   // Beaker evaluator cell",
+                    "        },",
+                    "        atomic_data = {",
+                    "            \"namespace\": \".atomic-data\",    // Namespace for select fields",
+                    "            \"periodic_table\": {",
+                    "                \"class\": \".periodic-table\", // Namespace for periodic table",
+                    "                \"colormap\": \"thermometer\",",
+                    "                \"text\": [",
+                    "                    \"All atomic properties\",",
+                    "                    \"for atomic property <q>{{name}}</q>\"",
+                    "                ]",
+                    "            },",
+                    "        },",
+                    "        paths = {",
+                    "            \"collections\": \"~/test/periodic-table/data\",",
+                    "            \"periodic_table\": \"~/test/periodic-table\"",
+                    "        };",
+                    "",
+                    "    /**",
+                    "     * Main loop",
+                    "     */",
+                    "    var main = function() {",
+                    "        // Initialize Atomic Data Client",
+                    "        instances.client = new AtomicData.Client(atomic_data);",
+                    "",
+                    "        // Initialize connector",
+                    "        connector.client = instances.client",
+                    "        instances.connector = new AtomicData.Connector(connector);",
+                    "",
+                    "        // Start main loop",
+                    "        instances.client.init(paths);",
+                    "    };",
+                    "",
+                    "    /**",
+                    "     * AtomicDataNotebook",
+                    "     */",
+                    "    var AtomicDataNotebook = function() {",
+                    "        /**",
+                    "         * Public methods",
+                    "         */",
+                    "        var backend = function() {",
+                    "            return instances.connector;",
+                    "        }",
+                    "",
+                    "        var frontend = function() {",
+                    "            return instances.client;",
+                    "        }",
+                    "",
+                    "        /**",
+                    "         * Initialization",
+                    "         */",
+                    "        return {",
+                    "            \"backend\": backend,",
+                    "            \"frontend\": frontend",
+                    "        };",
+                    "    };",
+                    "",
+                    "    // Declare classes into namespace",
+                    "    namespace.Notebook = new AtomicDataNotebook();",
+                    "",
+                    "    /**",
+                    "     * Run the main loop",
+                    "     */",
+                    "    main();",
+                    "})();"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "hidden": true,
+                "state": {},
+                "pluginName": "JavaScript"
+            },
+            "evaluatorReader": true,
+            "lineCount": 80,
+            "initialization": true
+        },
+        {
+            "id": "fetch_data",
+            "type": "code",
+            "evaluator": "IPython",
+            "input": {
+                "body": [
+                    "# Execute backend controller",
+                    "controller.execute()"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "hidden": true,
+                "state": {},
+                "pluginName": "IPython",
+                "shellId": "D6AB0868E05747479E7342FBBCD277FD"
+            },
+            "evaluatorReader": true,
+            "lineCount": 2,
+            "tags": "connector"
+        },
+        {
+            "id": "process_data",
+            "type": "code",
+            "evaluator": "JavaScript",
+            "input": {
+                "body": [
+                    "// Execute frontend controller by updating the backend JS model and calling the respective frontend functions",
+                    ";(function(){",
+                    "  var backend = AtomicData.Notebook.backend();",
+                    "  backend.update();",
+                    "}());"
+                ],
+                "hidden": true
+            },
+            "output": {
+                "hidden": true,
+                "state": {},
+                "pluginName": "JavaScript"
+            },
+            "evaluatorReader": true,
+            "lineCount": 5,
+            "tags": "connector"
+        }
+    ],
+    "namespace": {},
+    "locked": true
+}
diff --git a/example-data/periodic-table/data/electronic_affinity_neutral_atoms.json b/example-data/periodic-table/data/electronic_affinity_neutral_atoms.json
new file mode 100644
index 0000000..1e5af0a
--- /dev/null
+++ b/example-data/periodic-table/data/electronic_affinity_neutral_atoms.json
@@ -0,0 +1,944 @@
+{
+  "type": "nomad_info_data_json_2_0",
+  "mainFileUri": "file:///home/regler/OwnCloud/Promotion/Projekte/nomad-atomic-data/parser-atomic-data/tests/Experiment_electron_affinity_MKS.csv",
+  "parserInfo": {
+    "name":"AtomicDataParser",
+    "version":"1.2.0",
+    "parserId":"AtomicDataParserv1.1.0-6-g2cc2eb4",
+    "versionInfo":{
+      "nomadCoreVersion":{
+        "pythonCommonVersion":"1.3.0-7-g78469bb",
+        "name":"nomadCore",
+        "buildTime":"1486568683057",
+        "scalaVersion":"2.11.7",
+        "version":"1.7.0-21-g201fab3-dirty",
+        "metaInfoVersion":"1.6.0-42-g99dbf42",
+        "sbtVersion":"0.13.13"
+      },
+      "name":"atomicData",
+      "buildTime":"1486568683066",
+      "scalaVersion":"2.11.7",
+      "version":"v1.1.0-6-g2cc2eb4",
+      "sbtVersion":"0.13.13"
+    }
+  },
+  "sections": {
+    "section_atomic_data_collection-0": {
+    "type": "nomad_section_1_0",
+    "gIndex": 0,
+    "name": "section_atomic_data_collection",
+    "atomic_collection_name": "Experimental electron affinities for neutral atoms",
+    "atomic_collection_description": "The values for experimental electron affinity for neutral atoms are taken from\n\n- Lide, D. R.: CRC Handbook of Chemistry and Physics 86th ed. CRC Press, 2616 pp. (2005). [https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286]",
+    "sections": {
+      "section_atomic_property_method-0": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 0,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1103/PhysRevA.42.1405"
+        },
+      "section_atomic_property-0": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 0,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Fr",
+          "atomic_number": 87,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 7.370028E-20
+        },
+      "section_atomic_property_method-1": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 1,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1063/1.477771"
+        },
+      "section_atomic_property-1": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 1,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "As",
+          "atomic_number": 33,
+          "atomic_property_to_method_ref": 1,
+          "atomic_electron_affinity": 1.30417452E-19
+        },
+      "section_atomic_property_method-2": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 2,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1103/PhysRevLett.75.414"
+        },
+      "section_atomic_property-2": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 2,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Sr",
+          "atomic_number": 38,
+          "atomic_property_to_method_ref": 2,
+          "atomic_electron_affinity": 7.690464E-21
+        },
+      "section_atomic_property_method-3": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 3,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1063/1.463326"
+        },
+      "section_atomic_property-3": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 3,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Sb",
+          "atomic_number": 51,
+          "atomic_property_to_method_ref": 3,
+          "atomic_electron_affinity": 1.67588028E-19
+        },
+      "section_atomic_property_method-4": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 4,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1103/PhysRevA.58.2844"
+        },
+      "section_atomic_property-4": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 4,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "C",
+          "atomic_number": 6,
+          "atomic_property_to_method_ref": 4,
+          "atomic_electron_affinity": 2.02214181942E-19
+        },
+      "section_atomic_property-5": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 5,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Si",
+          "atomic_number": 14,
+          "atomic_property_to_method_ref": 4,
+          "atomic_electron_affinity": 2.22626275578E-19
+        },
+      "section_atomic_property-6": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 6,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Ge",
+          "atomic_number": 32,
+          "atomic_property_to_method_ref": 4,
+          "atomic_electron_affinity": 1.97502651216E-19
+        },
+      "section_atomic_property-7": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 7,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Sn",
+          "atomic_number": 50,
+          "atomic_property_to_method_ref": 4,
+          "atomic_electron_affinity": 1.78173150606E-19
+        },
+      "section_atomic_property_method-5": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 5,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1103/PhysRevA.57.R1493"
+        },
+      "section_atomic_property-8": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 8,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Al",
+          "atomic_number": 13,
+          "atomic_property_to_method_ref": 5,
+          "atomic_electron_affinity": 6.934715694E-20
+        },
+      "section_atomic_property_method-6": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 6,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "CRC-handbook"
+        },
+      "section_atomic_property-9": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 9,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Ac",
+          "atomic_number": 89,
+          "atomic_property_to_method_ref": 6,
+          "atomic_electron_affinity": 5.60763E-20
+        },
+      "section_atomic_property_method-7": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 7,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1088/0953-4075/25/8/012"
+        },
+      "section_atomic_property-10": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 10,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "I",
+          "atomic_number": 53,
+          "atomic_property_to_method_ref": 7,
+          "atomic_electron_affinity": 4.90112790066E-19
+        },
+      "section_atomic_property_method-8": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 8,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1103/PhysRevA.40.3698"
+        },
+      "section_atomic_property-11": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 11,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "F",
+          "atomic_number": 9,
+          "atomic_property_to_method_ref": 8,
+          "atomic_electron_affinity": 5.44931699202E-19
+        },
+      "section_atomic_property-12": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 12,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Br",
+          "atomic_number": 35,
+          "atomic_property_to_method_ref": 8,
+          "atomic_electron_affinity": 5.38907342184E-19
+        },
+      "section_atomic_property_method-9": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 9,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1088/0953-4075/31/11/002"
+        },
+      "section_atomic_property-13": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 13,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Yb",
+          "atomic_number": 70,
+          "atomic_property_to_method_ref": 9,
+          "atomic_electron_affinity": 3.20436E-21
+        },
+      "section_atomic_property_method-10": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 10,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1063/1.465868,10.1063/1.459475,10.1063/1.452170"
+        },
+      "section_atomic_property-14": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 14,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Cu",
+          "atomic_number": 29,
+          "atomic_property_to_method_ref": 10,
+          "atomic_electron_affinity": 1.9786923E-19
+        },
+      "section_atomic_property-15": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 15,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "W",
+          "atomic_number": 74,
+          "atomic_property_to_method_ref": 10,
+          "atomic_electron_affinity": 1.3057767E-19
+        },
+      "section_atomic_property_method-11": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 11,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1088/0953-4075/31/8/003"
+        },
+      "section_atomic_property-16": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 16,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Ga",
+          "atomic_number": 31,
+          "atomic_property_to_method_ref": 11,
+          "atomic_electron_affinity": 6.889374E-20
+        },
+      "section_atomic_property_method-12": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 12,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1088/0953-4075/31/20/002"
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+    "atomic_collection_description": "The values for experimental electron affinity for neutral atoms are taken from\n\n- Lide, D. R.: CRC Handbook of Chemistry and Physics 86th ed. CRC Press, 2616 pp. (2005). [https://www.crcpress.com/CRC-Handbook-of-Chemistry-and-Physics-97th-Edition/Haynes/p/book/9781498754286]"
+  }},
+  "parserStatus": "ParseSuccess"
+}
\ No newline at end of file
diff --git a/example-data/periodic-table/data/extended_binaries_dimers_atoms.json b/example-data/periodic-table/data/extended_binaries_dimers_atoms.json
new file mode 100644
index 0000000..0968ece
--- /dev/null
+++ b/example-data/periodic-table/data/extended_binaries_dimers_atoms.json
@@ -0,0 +1,2269 @@
+{
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+  "mainFileUri": "file:///home/regler/OwnCloud/Promotion/Projekte/nomad-atomic-data/parser-atomic-data/tests/ExtendedBinaries_Dimers_Atoms_new.csv",
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+    "type": "nomad_section_1_0",
+    "gIndex": 0,
+    "name": "section_atomic_data_collection",
+    "atomic_collection_name": "Extended binaries, dimers and atoms",
+    "atomic_collection_description": "This collection provides data for extended binaries, dimers, and atoms. It contains atom property information for rock-salt and zincblende crystal lattice structures, octet (I/II/III)-(V/VI/VII) binary materials, other eight-electron binaries using possible valences of d-metals and f-elements, and octet binaries from John and Bloch's paper:\n\n- John, J. & Bloch, A. N.: Quantum-Defect Electronegativity Scale for Nontransition Elements. Physical Review Letters, American Physical Society, 33, 1095-1098 (1974). DOI: 10.1103/PhysRevLett.33.1095 .\n\nThe atomic properties in this collection are obtained from:\n\n- Ghiringhelli, L. M.; Vybiral, J.; Levchenko, S. V.; Draxl, C. & Scheffler: M. Big Data of Materials Science: Critical Role of the Descriptor. Physical Review Letters, American Physical Society 114, 105503 (2015). DOI: 10.1103/PhysRevLett.114.105503 .",
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+          "atomic_element_symbol": "At",
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+          "atomic_element_symbol": "Rn",
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+      "section_atomic_property-86": {
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+          "atomic_element_symbol": "Fr",
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+          "atomic_r_homo_anion": 3.3E-10,
+          "atomic_number": 87,
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+        },
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+          "references": {
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+          "atomic_element_symbol": "Ra",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 2.64E-10,
+          "atomic_number": 88,
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+          "atomic_electron_affinity": 5.33364566837E-20
+        },
+      "section_atomic_property-88": {
+          "type": "nomad_section_1_0",
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+          "atomic_element_symbol": "Ac",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 2.32E-10,
+          "atomic_number": 89,
+          "atomic_r_homo": 1.8700000000000003E-10,
+          "atomic_ionization_potential": -8.368488451496001E-19,
+          "atomic_r_homo_cation": 1.65E-10,
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+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 6.9534461402E-21
+        },
+      "section_atomic_property-89": {
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+          "name": "section_atomic_property",
+          "gIndex": 89,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Th",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 8.7E-11,
+          "atomic_number": 90,
+          "atomic_r_homo": 1.2300000000000001E-10,
+          "atomic_ionization_potential": -9.180631734553E-19,
+          "atomic_r_homo_cation": 6.6E-11,
+          "atomic_mulliken_electronegativity": 4.860843374367E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": -5.4105501418100004E-20
+        },
+      "section_atomic_property-90": {
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+          "name": "section_atomic_property",
+          "gIndex": 90,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Pa",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 1.74E-10,
+          "atomic_number": 91,
+          "atomic_r_homo": 8.5E-11,
+          "atomic_ionization_potential": -8.468143831662001E-19,
+          "atomic_r_homo_cation": 8.2E-11,
+          "atomic_mulliken_electronegativity": 4.2425634514400004E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": -1.6983071218E-21
+        },
+      "section_atomic_property-91": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 91,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "U",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 1.7500000000000002E-10,
+          "atomic_number": 92,
+          "atomic_r_homo": 1.61E-10,
+          "atomic_ionization_potential": -8.917073695368E-19,
+          "atomic_r_homo_cation": 7.8E-11,
+          "atomic_mulliken_electronegativity": 4.0760973099729996E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 7.64718857769E-20
+        },
+      "section_atomic_property-92": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 92,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Np",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 9.0E-11,
+          "atomic_number": 93,
+          "atomic_r_homo": 7.3E-11,
+          "atomic_ionization_potential": -1.0312889888304E-18,
+          "atomic_r_homo_cation": 7.600000000000001E-11,
+          "atomic_mulliken_electronegativity": 4.446200088403E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 1.4204897114980002E-19
+        },
+      "section_atomic_property-93": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 93,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Pu",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 9.2E-11,
+          "atomic_number": 94,
+          "atomic_r_homo": 7.600000000000001E-11,
+          "atomic_ionization_potential": -1.1216837886530001E-18,
+          "atomic_r_homo_cation": 7.3E-11,
+          "atomic_mulliken_electronegativity": 4.764392347261E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 1.6880531920080002E-19
+        },
+      "section_atomic_property-94": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 94,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Am",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 7.5E-11,
+          "atomic_number": 95,
+          "atomic_r_homo": 7.2E-11,
+          "atomic_ionization_potential": -1.1011599073036999E-18,
+          "atomic_r_homo_cation": 7.1E-11,
+          "atomic_mulliken_electronegativity": 4.569727898866E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 1.872303492958E-19
+        },
+      "section_atomic_property-95": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 95,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Cm",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 7.0E-11,
+          "atomic_number": 96,
+          "atomic_r_homo": 6.9E-11,
+          "atomic_ionization_potential": 2.687651129075E-19,
+          "atomic_r_homo_cation": 6.800000000000001E-11,
+          "atomic_mulliken_electronegativity": -2.691336135094E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 2.695181358766E-19
+        },
+      "section_atomic_property-96": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 96,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Bk",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 6.9E-11,
+          "atomic_number": 97,
+          "atomic_r_homo": 6.6E-11,
+          "atomic_ionization_potential": -1.0694047684790999E-18,
+          "atomic_r_homo_cation": 6.6E-11,
+          "atomic_mulliken_electronegativity": 4.453089447482E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 1.7878687898269998E-19
+        },
+      "section_atomic_property-97": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 97,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Cf",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 6.800000000000001E-11,
+          "atomic_number": 98,
+          "atomic_r_homo": 6.4E-11,
+          "atomic_ionization_potential": -1.0562829426984E-18,
+          "atomic_r_homo_cation": 6.4E-11,
+          "atomic_mulliken_electronegativity": 4.734912299109E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 1.0928446111130002E-19
+        },
+      "section_atomic_property-98": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 98,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Es",
+          "atomic_charge": 0.0,
+          "atomic_r_homo_anion": 6.4E-11,
+          "atomic_number": 99,
+          "atomic_r_homo": 6.2E-11,
+          "atomic_ionization_potential": -1.0447472716824E-18,
+          "atomic_mulliken_electronegativity": 4.852672274064E-19,
+          "atomic_property_to_method_ref": 0,
+          "atomic_electron_affinity": 7.42288386349E-20
+        }},
+    "atomic_collection_name": "Extended binaries, dimers and atoms",
+    "atomic_collection_description": "This collection provides data for extended binaries, dimers, and atoms. It contains atom property information for rock-salt and zincblende crystal lattice structures, octet (I/II/III)-(V/VI/VII) binary materials, other eight-electron binaries using possible valences of d-metals and f-elements, and octet binaries from John and Bloch's paper:\n\n- John, J. & Bloch, A. N.: Quantum-Defect Electronegativity Scale for Nontransition Elements. Physical Review Letters, American Physical Society, 33, 1095-1098 (1974). DOI: 10.1103/PhysRevLett.33.1095 .\n\nThe atomic properties in this collection are obtained from:\n\n- Ghiringhelli, L. M.; Vybiral, J.; Levchenko, S. V.; Draxl, C. & Scheffler: M. Big Data of Materials Science: Critical Role of the Descriptor. Physical Review Letters, American Physical Society 114, 105503 (2015). DOI: 10.1103/PhysRevLett.114.105503 ."
+  }},
+  "parserStatus": "ParseSuccess"
+}
\ No newline at end of file
diff --git a/example-data/periodic-table/data/static_polarization.json b/example-data/periodic-table/data/static_polarization.json
new file mode 100644
index 0000000..278880e
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+++ b/example-data/periodic-table/data/static_polarization.json
@@ -0,0 +1,5782 @@
+{
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+    "atomic_collection_description": "This collection includes experimental and theoretically derived values for isotropic static polarizability as complied by Prof. Peter Schwerdtfeger.\n\n- Schwerdtfeger, P.: Table of experimental and calculated static dipole polarizabilities for the electronic ground states of the neutral elements (in atomic units). Centre for Theoretical Chemistry and Physics, The New Zealand Institute for Advanced Study (2014). [http://ctcp.massey.ac.nz/Tablepol2014.pdf]\n\nNot all published values are compiled, only the most accurate ones. There is some confusion about the experimental data listed in the CRC Handbook of Chemistry and Physics taken from Miller and Bederson. Some of the data are not experimental values as indicated, but from LDA calculations of Doolen, which are listed here as well.\n\nA more recent review by Mitroy, Safronova and Clark is highly recommended:\n\n- Mitroy, J.; Safronova, M. S. & Clark, C. W: Theory and applications of atomic and ionic polarizabilities. Journal of Physics B: Atomic, Molecular and Optical Physics 43, 202001 (2010). DOI: 10.1088/0953-4075/43/20/202001 .",
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+          "atomic_element_symbol": "Sn",
+          "atomic_number": 50,
+          "atomic_isotropic_polarizability": 7.89824463326744E-30,
+          "atomic_spin_multiplicity": 3,
+          "atomic_property_to_method_ref": 210
+        },
+      "section_atomic_property_method-211": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
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+          "references": {
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+          "atomic_term_symbol": "{1}^S_{0}",
+          "atomic_method": "relativistic_Douglas-Kroll+SO_CCSD(T)",
+          "atomic_property_source": "Theory",
+          "atomic_reference_DOI": "10.1103/PhysRevA.70.062501"
+        },
+      "section_atomic_property-279": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 279,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Ca",
+          "atomic_number": 20,
+          "atomic_isotropic_polarizability": 2.35020937867958E-29,
+          "atomic_spin_multiplicity": 1,
+          "atomic_property_to_method_ref": 211
+        },
+      "section_atomic_property_method-212": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 212,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_term_symbol": "{2}^S_{0}",
+          "atomic_property_source": "Experiment",
+          "atomic_reference_DOI": "10.1063/1.1713942"
+        },
+      "section_atomic_property-280": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 280,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "He",
+          "atomic_number": 2,
+          "atomic_isotropic_polarizability": 2.05043172590097E-31,
+          "atomic_spin_multiplicity": 1,
+          "atomic_property_to_method_ref": 212
+        },
+      "section_atomic_property_method-213": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 213,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_term_symbol": "{4}^F_{9/2}",
+          "atomic_method": "relativistic_Dirac_LDA",
+          "atomic_property_source": "Theory",
+          "atomic_reference_DOI": "10.1088/0031-8949/36/1/012"
+        },
+      "section_atomic_property-281": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 281,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Co",
+          "atomic_number": 27,
+          "atomic_isotropic_polarizability": 7.55741981794821E-30,
+          "atomic_spin_multiplicity": 4,
+          "atomic_property_to_method_ref": 213
+        },
+      "section_atomic_property_method-214": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 214,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_term_symbol": "5f^{7}6d^{1}",
+          "atomic_method": "R, Dirac, LDA",
+          "atomic_property_source": "Theory",
+          "atomic_reference_DOI": "10.1088/0031-8949/36/1/012"
+        },
+      "section_atomic_property-282": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 282,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_element_symbol": "Cm",
+          "atomic_number": 96,
+          "atomic_isotropic_polarizability": 2.296862885847E-29,
+          "atomic_spin_multiplicity": 9,
+          "atomic_property_to_method_ref": 214
+        }},
+    "atomic_collection_name": "Experimental and theoretically derived values for isotropic static polarizability",
+    "atomic_collection_description": "This collection includes experimental and theoretically derived values for isotropic static polarizability as complied by Prof. Peter Schwerdtfeger.\n\n- Schwerdtfeger, P.: Table of experimental and calculated static dipole polarizabilities for the electronic ground states of the neutral elements (in atomic units). Centre for Theoretical Chemistry and Physics, The New Zealand Institute for Advanced Study (2014). [http://ctcp.massey.ac.nz/Tablepol2014.pdf]\n\nNot all published values are compiled, only the most accurate ones. There is some confusion about the experimental data listed in the CRC Handbook of Chemistry and Physics taken from Miller and Bederson. Some of the data are not experimental values as indicated, but from LDA calculations of Doolen, which are listed here as well.\n\nA more recent review by Mitroy, Safronova and Clark is highly recommended:\n\n- Mitroy, J.; Safronova, M. S. & Clark, C. W: Theory and applications of atomic and ionic polarizabilities. Journal of Physics B: Atomic, Molecular and Optical Physics 43, 202001 (2010). DOI: 10.1088/0953-4075/43/20/202001 ."
+  }},
+  "parserStatus": "ParseSuccess"
+}
\ No newline at end of file
diff --git a/example-data/periodic-table/data/vdw_coefficients.json b/example-data/periodic-table/data/vdw_coefficients.json
new file mode 100644
index 0000000..b3cdd3a
--- /dev/null
+++ b/example-data/periodic-table/data/vdw_coefficients.json
@@ -0,0 +1,1674 @@
+{
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+  "mainFileUri": "file:///home/regler/OwnCloud/Promotion/Projekte/nomad-atomic-data/parser-atomic-data/tests/vdw.csv",
+  "parserInfo": {
+    "name":"AtomicDataParser",
+    "version":"1.2.0",
+    "parserId":"AtomicDataParserv1.1.0-6-g2cc2eb4",
+    "versionInfo":{
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+        "pythonCommonVersion":"1.3.0-7-g78469bb",
+        "name":"nomadCore",
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+        "scalaVersion":"2.11.7",
+        "version":"1.7.0-21-g201fab3-dirty",
+        "metaInfoVersion":"1.6.0-42-g99dbf42",
+        "sbtVersion":"0.13.13"
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+      "name":"atomicData",
+      "buildTime":"1486568683066",
+      "scalaVersion":"2.11.7",
+      "version":"v1.1.0-6-g2cc2eb4",
+      "sbtVersion":"0.13.13"
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+  "sections": {
+    "section_atomic_data_collection-0": {
+    "type": "nomad_section_1_0",
+    "gIndex": 0,
+    "name": "section_atomic_data_collection",
+    "atomic_collection_name": "Isotropic static polarizabilities and homo-atomic van der Waals coefficients for neutral free atoms",
+    "atomic_collection_description": "The majority of values such as isotropic static polarizability (in $bohr^3$) and the homo-atomic van der Waals coefficient (in $hartree \\cdot bohr^6$) for neutral free atoms are taken from:\n\n- Chu, X. & Dalgarno, A.: Linear response time-dependent density functional theory for van der Waals coefficients. The Journal of Chemical Physics 121, 9, 4083 (2004). DOI: 10.1063/1.1779576 .\n- Mitroy, J.; Safronova, M. S. & Clark, C. W: Theory and applications of atomic and ionic polarizabilities. Journal of Physics B: Atomic, Molecular and Optical Physics 43, 202001 (2010). DOI: 10.1088/0953-4075/43/20/202001 .\n\nThe rest of the elements are calculated using linear response coupled cluster single double theory with accurate basis. The van der Waals radii for the respective elements are defined as discussed in:\n\n- Tkatchenko, A. & Scheffler: Accurate Molecular Van Der Waals Interactions from Ground-State Electron Density and Free-Atom Reference Data. Physical Review Letters <strong>102</strong>, 073005 (2009). DOI: 10.1103/PhysRevLett.102.073005 .\n\nFor lanthanides and actinides, the $C_{6}$ coefficients are constructed to satisfy the valence electronic sum rule using the one-term formula which is equivalent to the two-point zeroth-order Pad\\'e approximant. Here, static polarizabilities are taken from:\n\n- Dzuba, V. A.; Kozlov, A.; Flambaum; V. V.: Scalar Static Polarizabilities of Lanthanides and Actinides. Physical Review A <strong>89</strong>, 042507 (2014). DOI: 10.1103/PhysRevA.89.042507 .",
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+          "atomic_reference_DOI": "10.1063/1.1779576,10.1088/0953-4075/43/20/202001,10.1103/PhysRevLett.102.073005",
+          "atomic_basis_set": "Def2-TZVPPD"
+        },
+      "section_atomic_property-99": {
+          "type": "nomad_section_1_0",
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+          "gIndex": 99,
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+          "atomic_number": 55,
+          "atomic_isotropic_polarizability": 6.329265388038574E-29,
+          "atomic_property_to_method_ref": 17
+        },
+      "section_atomic_property_method-18": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property_method",
+          "gIndex": 18,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_method": "SIC-TDDFT/LRCCSD",
+          "atomic_property_source": "Theory",
+          "atomic_reference_DOI": "10.1063/1.1779576,10.1088/0953-4075/43/20/202001,10.1103/PhysRevLett.102.073005",
+          "atomic_basis_set": "def2-qzvppd"
+        },
+      "section_atomic_property-100": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 100,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_vdw_radius": 1.9632474515857E-10,
+          "atomic_element_symbol": "K",
+          "atomic_charge": 0.0,
+          "atomic_isotropic_vdw_coefficient": 3.730767502338894E-76,
+          "atomic_number": 19,
+          "atomic_isotropic_polarizability": 4.3403301932864263E-29,
+          "atomic_property_to_method_ref": 18
+        },
+      "section_atomic_property-101": {
+          "type": "nomad_section_1_0",
+          "name": "section_atomic_property",
+          "gIndex": 101,
+          "references": {
+            "section_atomic_data_collection": 0},
+          "atomic_vdw_radius": 2.4606740296155E-10,
+          "atomic_element_symbol": "Ca",
+          "atomic_charge": 0.0,
+          "atomic_isotropic_vdw_coefficient": 2.1262598467268884E-76,
+          "atomic_number": 20,
+          "atomic_isotropic_polarizability": 2.3709553804227662E-29,
+          "atomic_property_to_method_ref": 18
+        }},
+    "atomic_collection_name": "Isotropic static polarizabilities and homo-atomic van der Waals coefficients for neutral free atoms",
+    "atomic_collection_description": "The majority of values such as isotropic static polarizability (in $bohr^3$) and the homo-atomic van der Waals coefficient (in $hartree \\cdot bohr^6$) for neutral free atoms are taken from:\n\n- Chu, X. & Dalgarno, A.: Linear response time-dependent density functional theory for van der Waals coefficients. The Journal of Chemical Physics 121, 9, 4083 (2004). DOI: 10.1063/1.1779576 .\n- Mitroy, J.; Safronova, M. S. & Clark, C. W: Theory and applications of atomic and ionic polarizabilities. Journal of Physics B: Atomic, Molecular and Optical Physics 43, 202001 (2010). DOI: 10.1088/0953-4075/43/20/202001 .\n\nThe rest of the elements are calculated using linear response coupled cluster single double theory with accurate basis. The van der Waals radii for the respective elements are defined as discussed in:\n\n- Tkatchenko, A. & Scheffler: Accurate Molecular Van Der Waals Interactions from Ground-State Electron Density and Free-Atom Reference Data. Physical Review Letters <strong>102</strong>, 073005 (2009). DOI: 10.1103/PhysRevLett.102.073005 .\n\nFor lanthanides and actinides, the $C_{6}$ coefficients are constructed to satisfy the valence electronic sum rule using the one-term formula which is equivalent to the two-point zeroth-order Pad\\'e approximant. Here, static polarizabilities are taken from:\n\n- Dzuba, V. A.; Kozlov, A.; Flambaum; V. V.: Scalar Static Polarizabilities of Lanthanides and Actinides. Physical Review A <strong>89</strong>, 042507 (2014). DOI: 10.1103/PhysRevA.89.042507 ."
+  }},
+  "parserStatus": "ParseSuccess"
+}
diff --git a/example-data/periodic-table/periodic_table.min.json b/example-data/periodic-table/periodic_table.min.json
new file mode 100644
index 0000000..6d55011
--- /dev/null
+++ b/example-data/periodic-table/periodic_table.min.json
@@ -0,0 +1 @@
+{"colormap":{"actinoid":"#669fc6","alkali metal":"#66d98c","alkaline earth metal":"#66c69f","halogen":"#66d98c","lanthanoid":"#669fc6","metal":"#66c69f","metalloid":"#66d098","noble gas":"#8cd966","nonmetal":"#66d98c","transition metal":"#66b3b3"},"elements":[{"atomic_number":1,"classification":"nonmetal","group":1,"name":"Hydrogen","period":1,"series":1,"symbol":"H"},{"atomic_number":2,"classification":"noble gas","group":18,"name":"Helium","period":1,"series":2,"symbol":"He"},{"atomic_number":3,"classification":"alkali metal","group":1,"name":"Lithium","period":2,"series":3,"symbol":"Li"},{"atomic_number":4,"classification":"alkaline earth 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