diff --git a/doc/magnetic_material_mammos.html b/doc/magnetic_material_mammos.html
index 2f9d93a..a986266 100644
--- a/doc/magnetic_material_mammos.html
+++ b/doc/magnetic_material_mammos.html
@@ -9,7 +9,7 @@
   <meta name="institution" content>
   <meta name="keywords" content="EMMO, materials
 science, modelling, characterisation, materials, ontology">
-  <meta name="dcterms.date" content="December 18, 2024">
+  <meta name="dcterms.date" content="December 21, 2024">
   <title>Magnetic Material Ontology</title>
   <style type="text/css">code{white-space: pre;}</style>
   <!--[if lt IE 9]>
@@ -411,7 +411,7 @@ <h3 class="institute">Magnetic Multiscale Modelling Suite
     
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" class="logo" width="128">
     
-        <h3 class="date">December 18, 2024</h3>
+        <h3 class="date">December 21, 2024</h3>
     
     
       </center>
@@ -444,6 +444,11 @@ <h3 class="date">December 18, 2024</h3>
 <li><a href="#overview" id="toc-overview">Overview</a>
 <ul>
 <li><a href="#magnet" id="toc-magnet">Magnet</a></li>
+<li><a href="#granular-microstructure" id="toc-granular-microstructure">Granular Microstructure</a></li>
+<li><a href="#magnetic-material" id="toc-magnetic-material">Magnetic
+material</a></li>
+<li><a href="#crystalline-magnetic-material" id="toc-crystalline-magnetic-material">Crystalline magnetic
+material</a></li>
 <li><a href="#classes" id="toc-classes">Classes</a></li>
 </ul></li>
 </ul></nav>
@@ -451,11 +456,53 @@ <h3 class="date">December 18, 2024</h3>
 
 
 <h1 id="overview">Overview</h1>
+<p>The MaMMoS magnetic materials ontology is a domain ontology which
+uses <a href="https://github.com/emmo-repo/EMMO">EMMO</a> as top level
+ontology. The magnetic material ontology reflects the hierarchical
+structure of the magnet. It reveals its physical parts at different
+length scales.</p>
 <h2 id="magnet">Magnet</h2>
+<p>A magnet is <em>functionally defined material</em>. Possible
+subclasses of a magnet are <em>bulk magnet</em>, <em>thin film
+magnet</em>, or <em>multilayer magnet</em>. A magnet may have a
+<em>granular microstructure</em>.</p>
 <figure>
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<g id="a_node5"><a xlink:href="https://w3id.org/emmo#EMMO_e4e80813_f379_4091_b017_ee059811f806" xlink:title="SizeDefinedMaterial">
<ellipse fill="#ffffcc" stroke="red" cx="560.67" cy="-43.36" rx="105.08" ry="18"/>
<text text-anchor="middle" x="560.67" y="-39.66" font-family="Times,serif" font-size="14.00">SizeDefinedMaterial</text>
</a>
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</g>
<!-- ThinfilmMagnet&#45;&gt;SizeDefinedMaterial -->
<g id="edge2" class="edge">
<title>ThinfilmMagnet&#45;&gt;SizeDefinedMaterial</title>
<path fill="none" stroke="black" d="M197.64,-131.12C214.1,-126.78 230.69,-120.24 244.38,-110.36 256.68,-101.48 249.61,-89.55 262.38,-81.36 295.37,-60.2 398.5,-64.35 437.38,-59.36 446.94,-58.14 456.91,-56.85 466.86,-55.55"/>
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<text text-anchor="middle" x="349.88" y="-85.16" font-family="Times,serif" font-size="14.00">isA</text>
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<!-- BulkMagnet -->
<g id="node2" class="node">
<title>BulkMagnet</title>
<g id="a_node2"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_d28323da-810f-5cbe-a770-eab7e7fdb493" xlink:title="BulkMagnet">
<ellipse fill="#ffffcc" stroke="black" cx="122.19" cy="-24.36" rx="67.69" ry="18"/>
<text text-anchor="middle" x="122.19" y="-20.66" font-family="Times,serif" font-size="14.00">BulkMagnet</text>
</a>
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<!-- BulkMagnet&#45;&gt;Magnet -->
<g id="edge7" class="edge">
<title>BulkMagnet&#45;&gt;Magnet</title>
<path fill="none" stroke="black" d="M190.02,-24.45C276,-25.07 416.77,-27.99 437.38,-40.36 450.71,-48.36 445.27,-58.55 455.38,-70.36 476.9,-95.5 506.18,-119.23 528.23,-135.54"/>
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<text text-anchor="middle" x="349.88" y="-44.16" font-family="Times,serif" font-size="14.00">isA</text>
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<!-- BulkMagnet&#45;&gt;SizeDefinedMaterial -->
<g id="edge8" class="edge">
<title>BulkMagnet&#45;&gt;SizeDefinedMaterial</title>
<path fill="none" stroke="black" d="M178.55,-14.42C241.55,-4.66 347.39,6.95 437.38,-6.36 460.69,-9.81 485.71,-16.77 507.01,-23.73"/>
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<text text-anchor="middle" x="349.88" y="-10.16" font-family="Times,serif" font-size="14.00">isA</text>
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<!-- MultilayerMagnet -->
<g id="node3" class="node">
<title>MultilayerMagnet</title>
<g id="a_node3"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_4ee603fc-7a1e-51f0-bf75-8e66f9a5539b" xlink:title="MultilayerMagnet">
<ellipse fill="#ffffcc" stroke="black" cx="122.19" cy="-212.36" rx="94.78" ry="18"/>
<text text-anchor="middle" x="122.19" y="-208.66" font-family="Times,serif" font-size="14.00">MultilayerMagnet</text>
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</g>
<!-- MultilayerMagnet&#45;&gt;ThinfilmMagnet -->
<g id="edge5" class="edge">
<title>MultilayerMagnet&#45;&gt;ThinfilmMagnet</title>
<path fill="none" stroke="darkgreen" stroke-dasharray="5,2" d="M122.19,-194.27C122.19,-186.19 122.19,-176.48 122.19,-167.49"/>
<polygon fill="darkgreen" stroke="darkgreen" points="125.69,-167.41 122.19,-157.41 118.69,-167.41 125.69,-167.41"/>
<text text-anchor="middle" x="111.69" y="-172.16" font-family="Times,serif" font-size="14.00">hasSpatialTile some</text>
</g>
<!-- MultilayerMagnet&#45;&gt;Magnet -->
<g id="edge3" class="edge">
<title>MultilayerMagnet&#45;&gt;Magnet</title>
<path fill="none" stroke="black" d="M201.73,-202.46C289.75,-191.37 430.08,-173.69 506.25,-164.09"/>
<polygon fill="none" stroke="black" points="507.08,-167.52 516.56,-162.79 506.2,-160.57 507.08,-167.52"/>
<text text-anchor="middle" x="349.88" y="-199.16" font-family="Times,serif" font-size="14.00">isA</text>
</g>
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<g id="node6" class="node">
<title>SpatialTiling</title>
<g id="a_node6"><a xlink:href="https://w3id.org/emmo#EMMO_8944581c_64da_46a9_be29_7074f7cc8098" xlink:title="SpatialTiling">
<ellipse fill="#ffffcc" stroke="red" cx="560.67" cy="-233.36" rx="69.59" ry="18"/>
<text text-anchor="middle" x="560.67" y="-229.66" font-family="Times,serif" font-size="14.00">SpatialTiling</text>
</a>
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</g>
<!-- MultilayerMagnet&#45;&gt;SpatialTiling -->
<g id="edge4" class="edge">
<title>MultilayerMagnet&#45;&gt;SpatialTiling</title>
<path fill="none" stroke="black" d="M214.42,-216.75C293.55,-220.56 406.83,-226.01 481.77,-229.61"/>
<polygon fill="none" stroke="black" points="481.93,-233.12 492.09,-230.11 482.27,-226.13 481.93,-233.12"/>
<text text-anchor="middle" x="349.88" y="-231.16" font-family="Times,serif" font-size="14.00">isA</text>
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<!-- SpacerLayer -->
<g id="node7" class="node">
<title>SpacerLayer</title>
<g id="a_node7"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_1b980f86-4116-5af8-bc45-14b44d88eeb5" xlink:title="SpacerLayer">
<ellipse fill="#ffffcc" stroke="red" cx="122.19" cy="-284.36" rx="69.59" ry="18"/>
<text text-anchor="middle" x="122.19" y="-280.66" font-family="Times,serif" font-size="14.00">SpacerLayer</text>
</a>
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<!-- MultilayerMagnet&#45;&gt;SpacerLayer -->
<g id="edge6" class="edge">
<title>MultilayerMagnet&#45;&gt;SpacerLayer</title>
<path fill="none" stroke="darkgreen" stroke-dasharray="5,2" d="M122.19,-230.53C122.19,-238.23 122.19,-247.39 122.19,-255.94"/>
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<text text-anchor="middle" x="111.69" y="-244.66" font-family="Times,serif" font-size="14.00">hasSpatialTile min 0</text>
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<!-- FunctionallyDefinedMaterial -->
<g id="node8" class="node">
<title>FunctionallyDefinedMaterial</title>
<g id="a_node8"><a xlink:href="https://w3id.org/emmo#EMMO_8820f251_ad36_43f4_a693_c0e86a89cc1f" xlink:title="FunctionallyDefinedMaterial">
<ellipse fill="#ffffcc" stroke="red" cx="867.6" cy="-157.36" rx="143.77" ry="18"/>
<text text-anchor="middle" x="867.6" y="-153.66" font-family="Times,serif" font-size="14.00">FunctionallyDefinedMaterial</text>
</a>
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</g>
<!-- Magnet&#45;&gt;FunctionallyDefinedMaterial -->
<g id="edge9" class="edge">
<title>Magnet&#45;&gt;FunctionallyDefinedMaterial</title>
<path fill="none" stroke="black" d="M606.99,-157.36C635.62,-157.36 674.45,-157.36 713.34,-157.36"/>
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<text text-anchor="middle" x="694.96" y="-161.16" font-family="Times,serif" font-size="14.00">isA</text>
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<g id="node9" class="node">
<title>GranularMicrostructure</title>
<g id="a_node9"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2" xlink:title="GranularMicrostructure">
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<text text-anchor="middle" x="122.19" y="-79.66" font-family="Times,serif" font-size="14.00">GranularMicrostructure</text>
</a>
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</g>
<!-- Magnet&#45;&gt;GranularMicrostructure -->
<g id="edge10" class="edge">
<title>Magnet&#45;&gt;GranularMicrostructure</title>
<path fill="none" stroke="darkgreen" d="M522.99,-146.92C498.82,-140.32 466.4,-132.01 437.38,-126.36 369.29,-113.12 292.13,-102.49 231.31,-95.12"/>
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<text text-anchor="middle" x="349.88" y="-130.16" font-family="Times,serif" font-size="14.00">hasSpatialPart exactly 1</text>
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<g id="node10" class="node">
<title>key1</title>
<text text-anchor="start" x="156.19" y="-369.16" font-family="Times,serif" font-weight="bold" font-size="14.00">isA</text>
<text text-anchor="start" x="64.19" y="-350.16" font-family="Times,serif" font-weight="bold" font-size="14.00">hasSpatialPart</text>
<text text-anchor="start" x="79.19" y="-330.16" font-family="Times,serif" font-size="14.00">hasSpatialTile</text>
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<g id="node11" class="node">
<title>key2</title>
<text text-anchor="start" x="558.67" y="-368.16" font-family="Times,serif" font-size="14.00"> </text>
<text text-anchor="start" x="558.67" y="-349.16" font-family="Times,serif" font-size="14.00"> </text>
<text text-anchor="start" x="558.67" y="-330.16" font-family="Times,serif" font-size="14.00"> </text>
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<g id="edge11" class="edge">
<title>key1:e&#45;&gt;key2:w</title>
<path fill="none" stroke="black" d="M184.19,-372.36C345.91,-372.36 388.82,-372.36 545.67,-372.36"/>
<polygon fill="none" stroke="black" points="545.67,-375.86 555.67,-372.36 545.67,-368.86 545.67,-375.86"/>
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<!-- key1&#45;&gt;key2 -->
<g id="edge12" class="edge">
<title>key1:e&#45;&gt;key2:w</title>
<path fill="none" stroke="darkgreen" d="M184.19,-352.36C345.91,-352.36 388.82,-352.36 545.67,-352.36"/>
<polygon fill="darkgreen" stroke="darkgreen" points="545.67,-355.86 555.67,-352.36 545.67,-348.86 545.67,-355.86"/>
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<g id="edge13" class="edge">
<title>key1:e&#45;&gt;key2:w</title>
<path fill="none" stroke="darkgreen" stroke-dasharray="5,2" d="M184.19,-333.36C345.91,-333.36 388.82,-333.36 545.67,-333.36"/>
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<polygon fill="white" stroke="transparent" points="-4,4 -4,-408.5 1204.92,-408.5 1204.92,4 -4,4"/>
<!-- ThinfilmMagnet -->
<g id="node1" class="node">
<title>ThinfilmMagnet</title>
<g id="a_node1"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_613e4315-d58f-5b5d-82ce-8cb76bd1b0aa" xlink:title="ThinfilmMagnet">
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<text text-anchor="middle" x="335.88" y="-79.3" font-family="Times,serif" font-size="14.00">ThinfilmMagnet</text>
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<!-- Magnet -->
<g id="node2" class="node">
<title>Magnet</title>
<g id="a_node2"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_099b796d-3163-56c7-bc90-3a304256ca5d" xlink:title="Magnet">
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<text text-anchor="middle" x="750.36" y="-115.3" font-family="Times,serif" font-size="14.00">Magnet</text>
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<!-- ThinfilmMagnet&#45;&gt;Magnet -->
<g id="edge5" class="edge">
<title>ThinfilmMagnet&#45;&gt;Magnet</title>
<path fill="none" stroke="black" d="M411.98,-90.83C432.73,-92.92 455.27,-95.12 476.07,-97 551.78,-103.85 639.39,-110.72 694.58,-114.91"/>
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<text text-anchor="middle" x="551.57" y="-113.8" font-family="Times,serif" font-size="14.00">isA</text>
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<!-- SizeDefinedMaterial -->
<g id="node7" class="node">
<title>SizeDefinedMaterial</title>
<g id="a_node7"><a xlink:href="https://w3id.org/emmo#EMMO_e4e80813_f379_4091_b017_ee059811f806" xlink:title="SizeDefinedMaterial">
<ellipse fill="#ffffcc" stroke="red" cx="750.36" cy="-35" rx="105.08" ry="18"/>
<text text-anchor="middle" x="750.36" y="-31.3" font-family="Times,serif" font-size="14.00">SizeDefinedMaterial</text>
</a>
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<!-- ThinfilmMagnet&#45;&gt;SizeDefinedMaterial -->
<g id="edge6" class="edge">
<title>ThinfilmMagnet&#45;&gt;SizeDefinedMaterial</title>
<path fill="none" stroke="black" d="M418.14,-78.71C476.47,-75.03 556.84,-68.76 627.07,-59 642.45,-56.86 658.82,-54.04 674.41,-51.08"/>
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<text text-anchor="middle" x="551.57" y="-78.8" font-family="Times,serif" font-size="14.00">isA</text>
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<g id="node5" class="node">
<title>FunctionallyDefinedMaterial</title>
<g id="a_node5"><a xlink:href="https://w3id.org/emmo#EMMO_8820f251_ad36_43f4_a693_c0e86a89cc1f" xlink:title="FunctionallyDefinedMaterial">
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<text text-anchor="middle" x="1057.29" y="-115.3" font-family="Times,serif" font-size="14.00">FunctionallyDefinedMaterial</text>
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<!-- Magnet&#45;&gt;FunctionallyDefinedMaterial -->
<g id="edge1" class="edge">
<title>Magnet&#45;&gt;FunctionallyDefinedMaterial</title>
<path fill="none" stroke="black" d="M796.68,-119C825.31,-119 864.14,-119 903.03,-119"/>
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<text text-anchor="middle" x="884.65" y="-122.8" font-family="Times,serif" font-size="14.00">isA</text>
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<g id="node6" class="node">
<title>GranularMicrostructure</title>
<g id="a_node6"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2" xlink:title="GranularMicrostructure">
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<g id="edge2" class="edge">
<title>Magnet&#45;&gt;GranularMicrostructure</title>
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<g id="node3" class="node">
<title>MultilayerMagnet</title>
<g id="a_node3"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_4ee603fc-7a1e-51f0-bf75-8e66f9a5539b" xlink:title="MultilayerMagnet">
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<g id="edge9" class="edge">
<title>MultilayerMagnet&#45;&gt;ThinfilmMagnet</title>
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<g id="edge7" class="edge">
<title>MultilayerMagnet&#45;&gt;Magnet</title>
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<g id="node8" class="node">
<title>SpatialTiling</title>
<g id="a_node8"><a xlink:href="https://w3id.org/emmo#EMMO_8944581c_64da_46a9_be29_7074f7cc8098" xlink:title="SpatialTiling">
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<text text-anchor="middle" x="750.36" y="-229.3" font-family="Times,serif" font-size="14.00">SpatialTiling</text>
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<g id="edge8" class="edge">
<title>MultilayerMagnet&#45;&gt;SpatialTiling</title>
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<g id="node9" class="node">
<title>SpacerLayer</title>
<g id="a_node9"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_1b980f86-4116-5af8-bc45-14b44d88eeb5" xlink:title="SpacerLayer">
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</a>
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<g id="edge10" class="edge">
<title>MultilayerMagnet&#45;&gt;SpacerLayer</title>
<path fill="none" stroke="darkgreen" stroke-dasharray="5,2" d="M242.84,-191.11C152.85,-190.46 36.48,-199.78 83.69,-256.5 126.41,-307.82 205.65,-314.97 263.94,-312.08"/>
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<g id="node4" class="node">
<title>BulkMagnet</title>
<g id="a_node4"><a xlink:href="http://www.emmc.info/emmc-csa/magnetic_material#EMMO_d28323da-810f-5cbe-a770-eab7e7fdb493" xlink:title="BulkMagnet">
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</a>
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<g id="edge3" class="edge">
<title>BulkMagnet&#45;&gt;Magnet</title>
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<!-- BulkMagnet&#45;&gt;SizeDefinedMaterial -->
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" width="1024" alt="A Magnet and its parts." />
 <figcaption aria-hidden="true">A Magnet and its parts.</figcaption>
 </figure>
+<h2 id="granular-microstructure">Granular Microstructure</h2>
+<p>The spatial parts of the granular microstructure are the <em>main
+magnetic phase</em>, the <em>grain boundary phase</em>, and
+<em>secondary phase</em>.</p>
+<p>The granular microstructure constists of a <em>main magnetic
+phase</em>, possible <em>grain boundary phases</em> and <em>secondary
+phases</em>.</p>
+<figure>
+<img src="data:image/svg+xml;base64,<?xml version="1.0" encoding="UTF-8" standalone="no"?>
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" width="1024" alt="The granular microstructure of a magnet." />
+<figcaption aria-hidden="true">The granular microstructure of a
+magnet.</figcaption>
+</figure>
+<h2 id="magnetic-material">Magnetic material</h2>
+<p>The main magnetic phase is a <em>magnetic material</em>. A magnetic
+material has <em>intrinsic magnetic properties</em> and a <em>chemical
+composition</em>. A magnetic material can be amorphous or
+crystalline.</p>
+<figure>
+<img src="data:image/svg+xml;base64,<?xml version="1.0" encoding="UTF-8" standalone="no"?>
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+<figcaption aria-hidden="true">A magnetic material and its
+relations.</figcaption>
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+<h2 id="crystalline-magnetic-material">Crystalline magnetic
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" width="956" alt="A crystalline magnetic material." />
+<figcaption aria-hidden="true">A crystalline magnetic
+material.</figcaption>
+</figure>
 <h2 id="classes">Classes</h2>
 <h3 id="EMMO_98f7a685-fa5a-54f1-8504-f398047f3ab6">AbsolutePermeability</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_98f7a685-fa5a-54f1-8504-f398047f3ab6">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_98f7a685-fa5a-54f1-8504-f398047f3ab6</a></p>
@@ -485,6 +532,18 @@ <h3 id="EMMO_694b3915-3326-5fb2-87a1-20ccf1dc79dc">AmorphousMagneticMaterial</h3
 <li>is_a <a href="#EMMO_c5ca93ce-ad27-5f4a-95ef-aca0990c6937">MagneticMaterial</a></li>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_0afc19b0_2d43_4b3d_8da0_9ffb63bc1492">AmorphousMaterial</a></li>
 </ul>
+<h3 id="EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf">AmpereSquareMetrePerKilogram</h3>
+<p><strong>IRI:</strong> <a href="#EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf</a></p>
+<p><strong>elucidation:</strong> Unit of the magnetic moment per unit
+mass: Am²/kg</p>
+<p><strong>prefLabel:</strong> AmpereSquareMetrePerKilogram</p>
+<p><strong>Subclass of:</strong></p>
+<ul>
+<li>is_a <a href="https://w3id.org/emmo#EMMO_b081b346_7279_46ef_9a3d_2c088fcd79f4">MeasurementUnit</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_19d925d0_2cf1_40e5_a391_1a99d68409c9">hasDimensionString</a>
+value ‘<a href="T0%20L+2%20M-1%20I+1%20Θ0%20N0%20J0">T0 L+2 M-1 I+1 Θ0
+N0 J0</a>’</li>
+</ul>
 <h3 id="EMMO_cd58ebab-4351-5d0d-ad45-bbddd6efead3">AnisotropyField</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_cd58ebab-4351-5d0d-ad45-bbddd6efead3">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_cd58ebab-4351-5d0d-ad45-bbddd6efead3</a></p>
 <p><strong>elucidation:</strong> The anisotropy field Ha is defined as
@@ -510,11 +569,11 @@ <h3 id="EMMO_d28323da-810f-5cbe-a770-eab7e7fdb493">BulkMagnet</h3>
 <li>is_a <a href="#EMMO_099b796d-3163-56c7-bc90-3a304256ca5d">Magnet</a></li>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_e4e80813_f379_4091_b017_ee059811f806">SizeDefinedMaterial</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_f8f03807-d6b6-5ebf-8e0b-418311e8e1e5">ShapeAnisotropy</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e">DemagnetizingFactor</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1">SampleGeometry</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_f8f03807-d6b6-5ebf-8e0b-418311e8e1e5">ShapeAnisotropy</a></li>
 </ul>
 <h3 id="EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395">CellVolume</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395</a></p>
@@ -583,21 +642,21 @@ <h3 id="EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3">CrystalStructure</h3>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba">Property</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395">CellVolume</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_2ca16b3d-f83e-583c-8292-beb6473ea021">LatticeConstantBeta</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_b2a130c3-9688-5358-94ca-f226b85b3009">LatticeConstantAlpha</a></li>
+exactly 1 <a href="#EMMO_a1f03bbf-c503-5759-9a26-2562527c0db2">LatticeConstantB</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_a205766b-7c02-5c56-90e5-96c553c316c8">LatticeConstantGamma</a></li>
+exactly 1 <a href="#EMMO_ef314f95-f3b5-5cb7-ac56-7bfc54f0d955">LatticeConstantA</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_5d5fbcc0-2738-5cb8-9157-a0fbe50eebb6">SpaceGroup</a></li>
+exactly 1 <a href="#EMMO_a205766b-7c02-5c56-90e5-96c553c316c8">LatticeConstantGamma</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_9977edfa-2b42-55e4-bea0-f39fadca7126">LatticeConstantC</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_a1f03bbf-c503-5759-9a26-2562527c0db2">LatticeConstantB</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_ef314f95-f3b5-5cb7-ac56-7bfc54f0d955">LatticeConstantA</a></li>
+exactly 1 <a href="#EMMO_5d5fbcc0-2738-5cb8-9157-a0fbe50eebb6">SpaceGroup</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395">CellVolume</a></li>
+exactly 1 <a href="#EMMO_b2a130c3-9688-5358-94ca-f226b85b3009">LatticeConstantAlpha</a></li>
 </ul>
 <h3 id="EMMO_aaa107b8-4dd9-5fc8-b135-a604a0cb38b1">CrystallineMagneticMaterial</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_aaa107b8-4dd9-5fc8-b135-a604a0cb38b1">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_aaa107b8-4dd9-5fc8-b135-a604a0cb38b1</a></p>
@@ -630,9 +689,9 @@ <h3 id="EMMO_af109e05-abbd-5964-8e39-8249b9eda7da">CubicMagnetocrystallineAnisot
 <ul>
 <li>is_a <a href="#EMMO_3a63baaf-4d7c-5ea5-93ce-9c8917a3290c">MagneticAnisotropy</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_527989d5-7417-5d94-83bf-4db785827a88">MagnetocrystallineAnisotropyConstantK1c</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">MagnetocrystallineAnisotropyConstantK1c</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_527989d5-7417-5d94-83bf-4db785827a88">MagnetocrystallineAnisotropyConstantK1c</a></li>
 </ul>
 <h3 id="EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e">DemagnetizingFactor</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e</a></p>
@@ -749,13 +808,13 @@ <h3 id="EMMO_8a0c8d0a-3dc7-5f3f-ab20-24b38d188827">ExtrinsicMagneticProperties</
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba">Property</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_14a12902-9845-5be6-bd0b-511dcea31985">MagneticHysteresisProperties</a></li>
+min 0 <a href="#EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e">DemagnetizingFactor</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="https://w3id.org/emmo#EMMO_593ecc7c_250d_4e4d_8957_0170f3cc2154">RelativePermeability</a></li>
+exactly 1 <a href="#EMMO_14a12902-9845-5be6-bd0b-511dcea31985">MagneticHysteresisProperties</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_98f7a685-fa5a-54f1-8504-f398047f3ab6">AbsolutePermeability</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e">DemagnetizingFactor</a></li>
+min 0 <a href="https://w3id.org/emmo#EMMO_593ecc7c_250d_4e4d_8957_0170f3cc2154">RelativePermeability</a></li>
 </ul>
 <h3 id="EMMO_aa999d91-076f-512a-85a0-c2f751c083b1">GeometricShape</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_aa999d91-076f-512a-85a0-c2f751c083b1">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_aa999d91-076f-512a-85a0-c2f751c083b1</a></p>
@@ -798,14 +857,14 @@ <h3 id="EMMO_b0f0e57e-464d-562f-80ec-b216c92d5e88">Grain</h3>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_0bb3b434_73aa_428f_b4e8_2a2468648e19">Crystal</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="https://w3id.org/emmo#EMMO_7efd64d1_05a1_49cd_a7f0_783ca050d4f3">ChemicalComposition</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3">CrystalStructure</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="https://w3id.org/emmo#EMMO_c1c8ac3c_8a1c_4777_8e0b_14c1f9f9b0c6">Diameter</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 (<a href="#EMMO_4f709756-86ee-5307-880a-696d08ae9732">CrystallographicOrientation</a>
 or <a href="#EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d">GrainMisalignmentAngle</a>)</li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3">CrystalStructure</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="https://w3id.org/emmo#EMMO_7efd64d1_05a1_49cd_a7f0_783ca050d4f3">ChemicalComposition</a></li>
 </ul>
 <h3 id="EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d">GrainMisalignmentAngle</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d</a></p>
@@ -858,11 +917,11 @@ <h3 id="EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2">GranularMicrostructure</h3>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_4207e895_8b83_4318_996a_72cfb32acd94">Material</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
+min 0 <a href="#EMMO_329e0b77-853d-5615-8df9-9bee0fd1189e">GrainboundaryPhase</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
 exactly 1 <a href="#EMMO_572b0885-bd40-51ad-8520-d5477c6b9990">MainMagneticPhase</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
 min 0 <a href="#EMMO_5394673b-027e-5afc-bc6f-f72df5ed40a1">SecondaryPhase</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
-min 0 <a href="#EMMO_329e0b77-853d-5615-8df9-9bee0fd1189e">GrainboundaryPhase</a></li>
 </ul>
 <h3 id="EMMO_75b995e0-2bac-5812-a7f6-f8c1731d1d5c">GranularStructure</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_75b995e0-2bac-5812-a7f6-f8c1731d1d5c">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_75b995e0-2bac-5812-a7f6-f8c1731d1d5c</a></p>
@@ -873,13 +932,13 @@ <h3 id="EMMO_75b995e0-2bac-5812-a7f6-f8c1731d1d5c">GranularStructure</h3>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_f1025834_0cd2_42a1_bfeb_13bec41c8655">CrystallineMaterial</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3">CrystalStructure</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_ada88738-c901-5d83-884b-5f84d27ce527">GrainSizeDistribution</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc">XrayDiffractionData</a></li>
+exactly 1 <a href="#EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3">CrystalStructure</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
 min 0 <a href="#EMMO_b0f0e57e-464d-562f-80ec-b216c92d5e88">Grain</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc">XrayDiffractionData</a></li>
 </ul>
 <h3 id="EMMO_eac1f731-95b1-5f31-ab94-2615535ea223">InducedMagneticAnisotropy</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_eac1f731-95b1-5f31-ab94-2615535ea223">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_eac1f731-95b1-5f31-ab94-2615535ea223</a></p>
@@ -923,15 +982,15 @@ <h3 id="EMMO_af8d3fb8-20fe-5f9f-9f85-fd298e26ad7e">IntrinsicMagneticProperties</
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba">Property</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-some <a href="#EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25">SpontaneousMagnetization</a></li>
+some <a href="#EMMO_57873439-dfa4-5b74-aec7-d530376ae11c">SpontaneousMagneticPolarisation</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 some <a href="#EMMO_c0a72108-de97-5dff-a830-e4b617adaeef">MagnetocrystallineAnisotropy</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 some <a href="https://w3id.org/emmo#EMMO_6b5af5a8_a2d8_4353_a1d6_54c9f778343d">CurieTemperature</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-some <a href="#EMMO_526ed2a5-a017-590e-8eb8-8a900f2b3b78">ExchangeStiffnessConstant</a></li>
+some <a href="#EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25">SpontaneousMagnetization</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-some <a href="#EMMO_57873439-dfa4-5b74-aec7-d530376ae11c">SpontaneousMagneticPolarisation</a></li>
+some <a href="#EMMO_526ed2a5-a017-590e-8eb8-8a900f2b3b78">ExchangeStiffnessConstant</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 some <a href="https://w3id.org/emmo#EMMO_f0b8bace_151e_4f54_8129_c180fd83ae44">NeelTemperature</a></li>
 </ul>
@@ -1125,13 +1184,13 @@ <h3 id="EMMO_099b796d-3163-56c7-bc90-3a304256ca5d">Magnet</h3>
 <p><strong>Subclass of:</strong></p>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_8820f251_ad36_43f4_a693_c0e86a89cc1f">FunctionallyDefinedMaterial</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc">XrayDiffractionData</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846">hasSpatialPart</a>
-exactly 1 <a href="#EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2">GranularMicrostructure</a></li>
+min 0 <a href="#EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2">GranularMicrostructure</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="https://w3id.org/emmo#EMMO_dd4b7d81_28a9_4801_8831_4cbab217e362">WorkpieceForming</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc">XrayDiffractionData</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_8a0c8d0a-3dc7-5f3f-ab20-24b38d188827">ExtrinsicMagneticProperties</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="https://w3id.org/emmo#EMMO_71d1c8f0_c6e3_44b5_a4b6_1b74ff35698a">MaterialsProcessing</a></li>
@@ -1168,27 +1227,27 @@ <h3 id="EMMO_14a12902-9845-5be6-bd0b-511dcea31985">MagneticHysteresisProperties<
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba">Property</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_fe101d1d-f1f7-54f8-886b-fa6d6052ce98">CoercivityHcExternal</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_234a6193-f057-556f-bfcd-38efde3aafc4">SwitchingFieldCoercivityExternal</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_bc54c47f-8560-516a-b95b-cce9f1b7344f">SwitchingFieldCoercivity</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926">MaximumEnergyProduct</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_ad0c038b-a09a-560c-b149-066de8f8e307">KneeField</a></li>
+exactly 1 <a href="#EMMO_8fc78216-4859-53c2-b41e-e38062b04054">Remanence</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_a4bc4536-f381-5bcd-b6ca-34fb1a913efd">CoercivityBHcExternal</a></li>
+min 0 <a href="#EMMO_fe101d1d-f1f7-54f8-886b-fa6d6052ce98">CoercivityHcExternal</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_538226cb-bebb-53e5-bf37-0f12226228be">RemanentMagneticPolarization</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_ad0c038b-a09a-560c-b149-066de8f8e307">KneeField</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_69772e86-d7fb-5b43-9cd4-2f0770c6701f">CoercivityBHc</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926">MaximumEnergyProduct</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_0d67d6c5-a8a7-57d4-930a-e99412baa2c2">CoercivityHc</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_45a36799-2309-5097-969f-4e5c002ae2f0">KneeFieldExternal</a></li>
+min 0 <a href="#EMMO_a4bc4536-f381-5bcd-b6ca-34fb1a913efd">CoercivityBHcExternal</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_8fc78216-4859-53c2-b41e-e38062b04054">Remanence</a></li>
+min 0 <a href="#EMMO_234a6193-f057-556f-bfcd-38efde3aafc4">SwitchingFieldCoercivityExternal</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_45a36799-2309-5097-969f-4e5c002ae2f0">KneeFieldExternal</a></li>
 </ul>
 <h3 id="EMMO_c5ca93ce-ad27-5f4a-95ef-aca0990c6937">MagneticMaterial</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_c5ca93ce-ad27-5f4a-95ef-aca0990c6937">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_c5ca93ce-ad27-5f4a-95ef-aca0990c6937</a></p>
@@ -1206,6 +1265,21 @@ <h3 id="EMMO_c5ca93ce-ad27-5f4a-95ef-aca0990c6937">MagneticMaterial</h3>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_af8d3fb8-20fe-5f9f-9f85-fd298e26ad7e">IntrinsicMagneticProperties</a></li>
 </ul>
+<h3 id="EMMO_8ffd7d16-848a-5e89-a553-0b5bb99971c4">MagneticMomementPerUnitMass</h3>
+<p><strong>IRI:</strong> <a href="#EMMO_8ffd7d16-848a-5e89-a553-0b5bb99971c4">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_8ffd7d16-848a-5e89-a553-0b5bb99971c4</a></p>
+<p><strong>elucidation:</strong> Magnetic moment per unit mass,
+sigma</p>
+<p><strong>altLabel:</strong> sigma, MassMagnetization,
+SpecificMagneticMoment</p>
+<p><strong>comment:</strong> The magnetization is obtained by
+multiplying sigma with the density</p>
+<p><strong>prefLabel:</strong> MagneticMomementPerUnitMass</p>
+<p><strong>Subclass of:</strong></p>
+<ul>
+<li>is_a <a href="https://w3id.org/emmo#EMMO_af794e9d_dc7d_4756_83e1_2cd0e2ec864e">ElectromagneticQuantity</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_bed1d005_b04e_4a90_94cf_02bc678a8569">hasMeasurementUnit</a>
+some <a href="#EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf">AmpereSquareMetrePerKilogram</a></li>
+</ul>
 <h3 id="EMMO_c0a72108-de97-5dff-a830-e4b617adaeef">MagnetocrystallineAnisotropy</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_c0a72108-de97-5dff-a830-e4b617adaeef">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_c0a72108-de97-5dff-a830-e4b617adaeef</a></p>
 <p><strong>elucidation:</strong> Magnetocrystalline anisotropy is an
@@ -1239,10 +1313,10 @@ <h3 id="EMMO_2bb87117-30f9-5b3a-b406-731836a3902f">MagnetocrystallineAnisotropyC
 <ul>
 <li>is_a <a href="#EMMO_56258d3a-f2ee-554e-af99-499dd8620457">EnergyDensity</a></li>
 </ul>
-<h3 id="EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">MagnetocrystallineAnisotropyConstantK1c</h3>
-<p><strong>IRI:</strong> <a href="#EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234</a></p>
-<p><strong>elucidation:</strong> The magnetocrystalline constant K2c for
-cubic crystals</p>
+<h3 id="EMMO_527989d5-7417-5d94-83bf-4db785827a88">MagnetocrystallineAnisotropyConstantK1c</h3>
+<p><strong>IRI:</strong> <a href="#EMMO_527989d5-7417-5d94-83bf-4db785827a88">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_527989d5-7417-5d94-83bf-4db785827a88</a></p>
+<p><strong>elucidation:</strong> The magnetocrystalline constant K1c for
+cubic crystals.</p>
 <p><strong>altLabel:</strong> K1</p>
 <p><strong>comment:</strong> Ea =
 K1c(a1²a2²+a2²a3²+a1²a3²)+K1c(a1²a2²a3²) where Ea is the anisotropy
@@ -1255,10 +1329,10 @@ <h3 id="EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">MagnetocrystallineAnisotropyC
 <ul>
 <li>is_a <a href="#EMMO_56258d3a-f2ee-554e-af99-499dd8620457">EnergyDensity</a></li>
 </ul>
-<h3 id="EMMO_527989d5-7417-5d94-83bf-4db785827a88">MagnetocrystallineAnisotropyConstantK1c</h3>
-<p><strong>IRI:</strong> <a href="#EMMO_527989d5-7417-5d94-83bf-4db785827a88">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_527989d5-7417-5d94-83bf-4db785827a88</a></p>
-<p><strong>elucidation:</strong> The magnetocrystalline constant K1c for
-cubic crystals.</p>
+<h3 id="EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">MagnetocrystallineAnisotropyConstantK1c</h3>
+<p><strong>IRI:</strong> <a href="#EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234</a></p>
+<p><strong>elucidation:</strong> The magnetocrystalline constant K2c for
+cubic crystals</p>
 <p><strong>altLabel:</strong> K1</p>
 <p><strong>comment:</strong> Ea =
 K1c(a1²a2²+a2²a3²+a1²a3²)+K1c(a1²a2²a3²) where Ea is the anisotropy
@@ -1327,6 +1401,21 @@ <h3 id="EMMO_572b0885-bd40-51ad-8520-d5477c6b9990">MainMagneticPhase</h3>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 some <a href="https://w3id.org/emmo#EMMO_a8eb87b5_4d10_4137_a75c_e04ee59ca095">VolumeFraction</a></li>
 </ul>
+<h3 id="EMMO_49768356-1ec9-5316-adbc-81001ecd770f">MassSusceptibility</h3>
+<p><strong>IRI:</strong> <a href="#EMMO_49768356-1ec9-5316-adbc-81001ecd770f">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_49768356-1ec9-5316-adbc-81001ecd770f</a></p>
+<p><strong>elucidation:</strong> Ratio of the change of the magnetic
+moment per unit mass and the internal field: sigma = chi_m H</p>
+<p><strong>altLabel:</strong> chi_m</p>
+<p><strong>comment:</strong> magnetic susceptibility per mass
+density</p>
+<p><strong>prefLabel:</strong> MassSusceptibility</p>
+<p><strong>wikidataReference:</strong> <a href="https://www.wikidata.org/wiki/Q104655916">https://www.wikidata.org/wiki/Q104655916</a></p>
+<p><strong>Subclass of:</strong></p>
+<ul>
+<li>is_a <a href="https://w3id.org/emmo#EMMO_af794e9d_dc7d_4756_83e1_2cd0e2ec864e">ElectromagneticQuantity</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_bed1d005_b04e_4a90_94cf_02bc678a8569">hasMeasurementUnit</a>
+some <a href="https://w3id.org/emmo#CubicMetrePerKilogram">CubicMetrePerKilogram</a></li>
+</ul>
 <h3 id="EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926">MaximumEnergyProduct</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926</a></p>
 <p><strong>elucidation:</strong> The value of the maximum energy product
@@ -1365,16 +1454,16 @@ <h3 id="EMMO_4ee603fc-7a1e-51f0-bf75-8e66f9a5539b">MultilayerMagnet</h3>
 <ul>
 <li>is_a <a href="#EMMO_099b796d-3163-56c7-bc90-3a304256ca5d">Magnet</a></li>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_8944581c_64da_46a9_be29_7074f7cc8098">SpatialTiling</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1">SampleGeometry</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_b2282816_b7a3_44c6_b2cb_3feff1ceb7fe">hasSpatialTile</a>
 some <a href="#EMMO_613e4315-d58f-5b5d-82ce-8cb76bd1b0aa">ThinfilmMagnet</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_d70e364c-7ab7-5329-9964-17a5e45bbb9d">StackingSquence</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1">SampleGeometry</a></li>
+min 0 <a href="#EMMO_5be2f193-36d0-5aac-90b8-52db055d8252">Magnetoresistance</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_b2282816_b7a3_44c6_b2cb_3feff1ceb7fe">hasSpatialTile</a>
 min 0 <a href="#EMMO_1b980f86-4116-5af8-bc45-14b44d88eeb5">SpacerLayer</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_5be2f193-36d0-5aac-90b8-52db055d8252">Magnetoresistance</a></li>
 </ul>
 <h3 id="EMMO_1bda25f0-3b11-5547-a27c-4e3a638b740a">NonMagneticMaterial</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_1bda25f0-3b11-5547-a27c-4e3a638b740a">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_1bda25f0-3b11-5547-a27c-4e3a638b740a</a></p>
@@ -1453,9 +1542,9 @@ <h3 id="EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1">SampleGeometry</h3>
 <ul>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba">Property</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-exactly 1 <a href="#EMMO_0213900b-ab6d-56be-82fb-4db874974de1">GeometricalSize</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 exactly 1 <a href="#EMMO_aa999d91-076f-512a-85a0-c2f751c083b1">GeometricShape</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+exactly 1 <a href="#EMMO_0213900b-ab6d-56be-82fb-4db874974de1">GeometricalSize</a></li>
 </ul>
 <h3 id="EMMO_5394673b-027e-5afc-bc6f-f72df5ed40a1">SecondaryPhase</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_5394673b-027e-5afc-bc6f-f72df5ed40a1">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_5394673b-027e-5afc-bc6f-f72df5ed40a1</a></p>
@@ -1562,7 +1651,7 @@ <h3 id="EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25">SpontaneousMagnetization</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25</a></p>
 <p><strong>elucidation:</strong> The spontaneous magnetization, Ms, of a
 ferromagnet is the result of alignment of the magnetic moments of
-individual atoms. Ms exists within a domain of a ferromagnet.</p>
+individual atoms.. Ms exists within a domain of a ferromagnet.</p>
 <p><strong>IECEntry:</strong> <a href="https://www.electropedia.org/iev/iev.nsf/display?openform&amp;ievref=221-02-41">https://www.electropedia.org/iev/iev.nsf/display?openform&amp;ievref=221-02-41</a></p>
 <p><strong>altLabel:</strong> Ms</p>
 <p><strong>prefLabel:</strong> SpontaneousMagnetization</p>
@@ -1619,21 +1708,21 @@ <h3 id="EMMO_613e4315-d58f-5b5d-82ce-8cb76bd1b0aa">ThinfilmMagnet</h3>
 <li>is_a <a href="#EMMO_099b796d-3163-56c7-bc90-3a304256ca5d">Magnet</a></li>
 <li>is_a <a href="https://w3id.org/emmo#EMMO_e4e80813_f379_4091_b017_ee059811f806">SizeDefinedMaterial</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_c44c0546-452e-592f-b6bc-27a64e79244c">LocalReflectivity</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_6aac026a-3928-5c21-9bb6-94497607bef2">LocalXrayDiffractionData</a></li>
-<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_dbb7c1bc-034f-5f4b-9329-d23ed8915961">LocalLatticeConstantC</a></li>
+min 0 <a href="#EMMO_c6ed4948-e599-5f09-aa07-b70121c41fcf">LocalLatticeConstantA</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_eac1f731-95b1-5f31-ab94-2615535ea223">InducedMagneticAnisotropy</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_c6ed4948-e599-5f09-aa07-b70121c41fcf">LocalLatticeConstantA</a></li>
+min 0 <a href="#EMMO_efffe3e8-6bd8-5944-ba38-6facf656c61d">LocalThickness</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1">SampleGeometry</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
-min 0 <a href="#EMMO_efffe3e8-6bd8-5944-ba38-6facf656c61d">LocalThickness</a></li>
+min 0 <a href="#EMMO_6aac026a-3928-5c21-9bb6-94497607bef2">LocalXrayDiffractionData</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_c44c0546-452e-592f-b6bc-27a64e79244c">LocalReflectivity</a></li>
 <li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
 min 0 <a href="#EMMO_17f52ffb-c461-546a-8af6-299a506c8657">LocalCoercivity</a></li>
+<li><a href="https://w3id.org/emmo#EMMO_e1097637_70d2_4895_973f_2396f04fa204">hasProperty</a>
+min 0 <a href="#EMMO_dbb7c1bc-034f-5f4b-9329-d23ed8915961">LocalLatticeConstantC</a></li>
 </ul>
 <h3 id="EMMO_49a882d1-9ce7-522b-91e7-3a460f25f5ac">UniaxialAnisotropyConstant</h3>
 <p><strong>IRI:</strong> <a href="#EMMO_49a882d1-9ce7-522b-91e7-3a460f25f5ac">http://www.emmc.info/emmc-csa/magnetic_material#EMMO_49a882d1-9ce7-522b-91e7-3a460f25f5ac</a></p>
@@ -1718,6 +1807,13 @@ <h2 class="index">Index</h2>
 <li><a href="#overview" id="toc-overview">Overview</a>
 <ul>
 <li><a href="#magnet" id="toc-magnet">Magnet</a></li>
+<li><a href="#granular-microstructure"
+id="toc-granular-microstructure">Granular Microstructure</a></li>
+<li><a href="#magnetic-material" id="toc-magnetic-material">Magnetic
+material</a></li>
+<li><a href="#crystalline-magnetic-material"
+id="toc-crystalline-magnetic-material">Crystalline magnetic
+material</a></li>
 <li><a href="#classes" id="toc-classes">Classes</a></li>
 </ul></li>
 </ul>
diff --git a/doc/mammos.md b/doc/mammos.md
index 01151d3..1a32da7 100644
--- a/doc/mammos.md
+++ b/doc/mammos.md
@@ -2,9 +2,38 @@
 
 %HEADER Overview 
 
+The MaMMoS magnetic materials ontology is a domain ontology which uses [EMMO](https://github.com/emmo-repo/EMMO) as top level ontology. The magnetic material ontology reflects the hierarchical structure of the magnet. It reveals its physical parts at different length scales.
+
 %HEADER "Magnet" level=2  
+
+A magnet is *functionally defined material*. Possible subclasses of a magnet are *bulk magnet*, *thin film magnet*, or *multilayer magnet*.
+A magnet may have a *granular microstructure*. 
+
 %BRANCHFIG Magnet addnodes=1 parents=0 rankdir='LR' relations=isA,hasSpatialPart,hasSpatialTile edgelabels=1 caption='A Magnet and its parts.'
 
+%HEADER "Granular Microstructure" level=2  
+
+The spatial parts of the granular microstructure are
+the *main magnetic phase*, the *grain boundary phase*, and *secondary phase*.
+
+The granular microstructure constists of a *main magnetic phase*, possible *grain boundary phases* and *secondary phases*.  
+
+%BRANCHFIG GranularMicrostructure addnodes=1 parents=1 rankdir='LR' relations=isA,hasSpatialPart,hasSpatialTile edgelabels=1 caption='The granular microstructure of a magnet.'
+
+%HEADER "Magnetic material" level=2  
+
+The main magnetic phase is a *magnetic material*. A magnetic material has
+*intrinsic magnetic properties* and a *chemical composition*. A magnetic material can be amorphous
+or crystalline.
+
+%BRANCHFIG MagneticMaterial addnodes=1 parents=0 rankdir='LR' relations=all edgelabels=1 caption='A magnetic material and its relations.'
+
+%HEADER "Crystalline magnetic material" level=2  
+
+A *crystalline magnetic material* is a *granular structure*. Properties of the granular structure are a *crystal structure* and a *grain size distribution*. *X-ray diffraction data* may have been measured.
+
+%BRANCHFIG CrystallineMagneticMaterial addnodes=1 parents=1 rankdir='LR' relations=all edgelabels=1 caption='A crystalline magnetic material.'
+
 %% you may add options to the documentation of a branch:  
 %% (default values are listed below)  
 %% caption=''      %% will give "Granular Microstructure branch.  
diff --git a/magnetic_material_mammos.ttl b/magnetic_material_mammos.ttl
index 91d123e..bffb355 100644
--- a/magnetic_material_mammos.ttl
+++ b/magnetic_material_mammos.ttl
@@ -25,11 +25,26 @@ email: wilfried.hortschitz@donau-uni.ac.at
 :EMMO_405ae501-8898-59c0-b2db-0afa09d561f9 a owl:AnnotationProperty ;
     skos:prefLabel "wikipediaReference"@en .
 
+:EMMO_49768356-1ec9-5316-adbc-81001ecd770f a owl:Class ;
+    :EMMO_4d45da04-cf90-5d4a-bc11-f76fbd5b5036 "https://www.wikidata.org/wiki/Q104655916"^^rdf:PlainLiteral ;
+    rdfs:comment "magnetic susceptibility per mass density"@en ;
+    rdfs:subClassOf [ a owl:Restriction ;
+            owl:onProperty ns1:EMMO_bed1d005_b04e_4a90_94cf_02bc678a8569 ;
+            owl:someValuesFrom ns1:CubicMetrePerKilogram ],
+        ns1:EMMO_af794e9d_dc7d_4756_83e1_2cd0e2ec864e ;
+    skos:altLabel "chi_m"@en ;
+    skos:prefLabel "MassSusceptibility"@en ;
+    ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "Ratio of the change of the magnetic moment per unit mass and the internal field: sigma = chi_m H"@en .
+
 :EMMO_4d45da04-cf90-5d4a-bc11-f76fbd5b5036 a owl:AnnotationProperty ;
     skos:prefLabel "wikidataReference"@en .
 
 :EMMO_4ee603fc-7a1e-51f0-bf75-8e66f9a5539b a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
+            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
+            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
+        [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_b2282816_b7a3_44c6_b2cb_3feff1ceb7fe ;
             owl:someValuesFrom :EMMO_613e4315-d58f-5b5d-82ce-8cb76bd1b0aa ],
         [ a owl:Restriction ;
@@ -37,17 +52,13 @@ email: wilfried.hortschitz@donau-uni.ac.at
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_5be2f193-36d0-5aac-90b8-52db055d8252 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass :EMMO_1b980f86-4116-5af8-bc45-14b44d88eeb5 ;
             owl:onProperty ns1:EMMO_b2282816_b7a3_44c6_b2cb_3feff1ceb7fe ],
-        [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_5be2f193-36d0-5aac-90b8-52db055d8252 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         :EMMO_099b796d-3163-56c7-bc90-3a304256ca5d,
         ns1:EMMO_8944581c_64da_46a9_be29_7074f7cc8098 ;
     skos:prefLabel "MultilayerMagnet"@en ;
@@ -61,6 +72,16 @@ email: wilfried.hortschitz@donau-uni.ac.at
     skos:prefLabel "MagnetocrystallineAnisotropyConstantK2"@en ;
     ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "The magnetocrystalline constant K2 for tetragonal or hexagonal crystals."@en .
 
+:EMMO_8ffd7d16-848a-5e89-a553-0b5bb99971c4 a owl:Class ;
+    rdfs:comment "The magnetization is obtained by multiplying sigma with the density"@en ;
+    rdfs:subClassOf [ a owl:Restriction ;
+            owl:onProperty ns1:EMMO_bed1d005_b04e_4a90_94cf_02bc678a8569 ;
+            owl:someValuesFrom :EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf ],
+        ns1:EMMO_af794e9d_dc7d_4756_83e1_2cd0e2ec864e ;
+    skos:altLabel "sigma, MassMagnetization, SpecificMagneticMoment"^^rdf:PlainLiteral ;
+    skos:prefLabel "MagneticMomementPerUnitMass"@en ;
+    ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "Magnetic moment per unit mass, sigma"@en .
+
 :EMMO_ab8a0d3e-6d0f-599e-a119-a91aa99bd881 a owl:Class ;
     :EMMO_4d45da04-cf90-5d4a-bc11-f76fbd5b5036 "https://www.wikidata.org/wiki/Q691463"^^rdf:PlainLiteral ;
     rdfs:subClassOf ns1:EMMO_e59eb557_3a0f_4532_9984_deed22f94952 ;
@@ -100,15 +121,15 @@ sum of the external field H′ and the demagnetizing field Hd"""@en .
 
 :EMMO_d28323da-810f-5cbe-a770-eab7e7fdb493 a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass :EMMO_f8f03807-d6b6-5ebf-8e0b-418311e8e1e5 ;
+            owl:onClass :EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e ;
+            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
+            owl:onClass :EMMO_f8f03807-d6b6-5ebf-8e0b-418311e8e1e5 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         :EMMO_099b796d-3163-56c7-bc90-3a304256ca5d,
@@ -144,6 +165,8 @@ called the applied field."""@en .
 :EMMO_eb748e96-0aee-5b55-b6be-56b8c6bdaed6 a owl:AnnotationProperty ;
     skos:prefLabel "IECEntry"@en .
 
+ns1:EMMO_b23e7251_a488_4732_8268_027ad76d7e37 skos:altLabel "VolumeMagnetization"@en .
+
 :EMMO_0213900b-ab6d-56be-82fb-4db874974de1 a owl:Class ;
     :EMMO_405ae501-8898-59c0-b2db-0afa09d561f9 "https://en.wikipedia.org/wiki/Size"^^rdf:PlainLiteral ;
     rdfs:subClassOf [ a owl:Restriction ;
@@ -163,7 +186,7 @@ called the applied field."""@en .
         ns1:EMMO_af794e9d_dc7d_4756_83e1_2cd0e2ec864e ;
     skos:altLabel "Ms"^^rdf:PlainLiteral ;
     skos:prefLabel "SpontaneousMagnetization"@en ;
-    ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "The spontaneous magnetization, Ms, of a ferromagnet is the result of alignment of the magnetic moments of  individual atoms. Ms exists within a domain of a ferromagnet."@en .
+    ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "The spontaneous magnetization, Ms, of a ferromagnet is the result of alignment of the magnetic moments of individual atoms.. Ms exists within a domain of a ferromagnet."@en .
 
 :EMMO_0d67d6c5-a8a7-57d4-930a-e99412baa2c2 a owl:Class ;
     rdfs:subClassOf ns1:EMMO_0e78a4d4_b4e0_48e7_97d8_e7d41a85a54d ;
@@ -177,19 +200,19 @@ sometimes referred to as 'intrinsic' coercivity."""@en .
 :EMMO_14a12902-9845-5be6-bd0b-511dcea31985 a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_fe101d1d-f1f7-54f8-886b-fa6d6052ce98 ;
+            owl:onClass :EMMO_bc54c47f-8560-516a-b95b-cce9f1b7344f ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_234a6193-f057-556f-bfcd-38efde3aafc4 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
+            owl:onClass :EMMO_8fc78216-4859-53c2-b41e-e38062b04054 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
+            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_bc54c47f-8560-516a-b95b-cce9f1b7344f ;
+            owl:onClass :EMMO_fe101d1d-f1f7-54f8-886b-fa6d6052ce98 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926 ;
+            owl:onClass :EMMO_538226cb-bebb-53e5-bf37-0f12226228be ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
@@ -197,15 +220,11 @@ sometimes referred to as 'intrinsic' coercivity."""@en .
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_a4bc4536-f381-5bcd-b6ca-34fb1a913efd ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
-        [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_538226cb-bebb-53e5-bf37-0f12226228be ;
+            owl:onClass :EMMO_69772e86-d7fb-5b43-9cd4-2f0770c6701f ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_69772e86-d7fb-5b43-9cd4-2f0770c6701f ;
+            owl:onClass :EMMO_e1028129-c23e-57ac-9174-2f34ddbf3926 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:onClass :EMMO_0d67d6c5-a8a7-57d4-930a-e99412baa2c2 ;
@@ -213,12 +232,16 @@ sometimes referred to as 'intrinsic' coercivity."""@en .
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_45a36799-2309-5097-969f-4e5c002ae2f0 ;
+            owl:onClass :EMMO_a4bc4536-f381-5bcd-b6ca-34fb1a913efd ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_8fc78216-4859-53c2-b41e-e38062b04054 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_234a6193-f057-556f-bfcd-38efde3aafc4 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
+        [ a owl:Restriction ;
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_45a36799-2309-5097-969f-4e5c002ae2f0 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         ns1:EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba ;
     skos:prefLabel "MagneticHysteresisProperties"@en ;
     ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 """The essential practical characteristic of any ferromagnetic material is the irreversible nonlinear response of magnetization M to an imposed magnetic field H. This response is given by the hysteresis loop. The charactertics of hystereis loop are known as hysteresis properties.
@@ -437,35 +460,35 @@ Crystallography."""@en .
 :EMMO_613e4315-d58f-5b5d-82ce-8cb76bd1b0aa a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_c44c0546-452e-592f-b6bc-27a64e79244c ;
+            owl:onClass :EMMO_c6ed4948-e599-5f09-aa07-b70121c41fcf ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_6aac026a-3928-5c21-9bb6-94497607bef2 ;
+            owl:onClass :EMMO_eac1f731-95b1-5f31-ab94-2615535ea223 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_dbb7c1bc-034f-5f4b-9329-d23ed8915961 ;
+            owl:onClass :EMMO_efffe3e8-6bd8-5944-ba38-6facf656c61d ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_eac1f731-95b1-5f31-ab94-2615535ea223 ;
+            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_c6ed4948-e599-5f09-aa07-b70121c41fcf ;
+            owl:onClass :EMMO_6aac026a-3928-5c21-9bb6-94497607bef2 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 ;
+            owl:onClass :EMMO_c44c0546-452e-592f-b6bc-27a64e79244c ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_efffe3e8-6bd8-5944-ba38-6facf656c61d ;
+            owl:onClass :EMMO_17f52ffb-c461-546a-8af6-299a506c8657 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_17f52ffb-c461-546a-8af6-299a506c8657 ;
+            owl:onClass :EMMO_dbb7c1bc-034f-5f4b-9329-d23ed8915961 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         :EMMO_099b796d-3163-56c7-bc90-3a304256ca5d,
         ns1:EMMO_e4e80813_f379_4091_b017_ee059811f806 ;
@@ -512,20 +535,20 @@ BHc depends on sample shape and has to be corrected for the demagnetizing field.
 
 :EMMO_8a0c8d0a-3dc7-5f3f-ab20-24b38d188827 a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
+        [ a owl:Restriction ;
             owl:onClass :EMMO_14a12902-9845-5be6-bd0b-511dcea31985 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
-        [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass ns1:EMMO_593ecc7c_250d_4e4d_8957_0170f3cc2154 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass :EMMO_98f7a685-fa5a-54f1-8504-f398047f3ab6 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_0f2b5cc9-d00a-5030-8448-99ba6b7dfd1e ;
+            owl:onClass ns1:EMMO_593ecc7c_250d_4e4d_8957_0170f3cc2154 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         ns1:EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba ;
     skos:prefLabel "ExtrinsicMagneticProperties"@en ;
@@ -643,13 +666,13 @@ Given by its mean and standard deviation of a lognormal distribution"""@en .
 
 :EMMO_af109e05-abbd-5964-8e39-8249b9eda7da a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass :EMMO_527989d5-7417-5d94-83bf-4db785827a88 ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
-        [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass :EMMO_c4aefa50-a3d0-548d-96ea-dd863ba27234 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
+        [ a owl:Restriction ;
+            owl:onClass :EMMO_527989d5-7417-5d94-83bf-4db785827a88 ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
+            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         :EMMO_3a63baaf-4d7c-5ea5-93ce-9c8917a3290c ;
     skos:prefLabel "CubicMagnetocrystallineAnisotropy"^^rdf:PlainLiteral ;
     ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "Cubic crystals anisotropy"@en .
@@ -657,7 +680,7 @@ Given by its mean and standard deviation of a lognormal distribution"""@en .
 :EMMO_af8d3fb8-20fe-5f9f-9f85-fd298e26ad7e a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:someValuesFrom :EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25 ],
+            owl:someValuesFrom :EMMO_57873439-dfa4-5b74-aec7-d530376ae11c ],
         [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:someValuesFrom :EMMO_c0a72108-de97-5dff-a830-e4b617adaeef ],
@@ -666,10 +689,10 @@ Given by its mean and standard deviation of a lognormal distribution"""@en .
             owl:someValuesFrom ns1:EMMO_6b5af5a8_a2d8_4353_a1d6_54c9f778343d ],
         [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:someValuesFrom :EMMO_526ed2a5-a017-590e-8eb8-8a900f2b3b78 ],
+            owl:someValuesFrom :EMMO_032731f8-874d-5efb-9c9d-6dafaa17ef25 ],
         [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
-            owl:someValuesFrom :EMMO_57873439-dfa4-5b74-aec7-d530376ae11c ],
+            owl:someValuesFrom :EMMO_526ed2a5-a017-590e-8eb8-8a900f2b3b78 ],
         [ a owl:Restriction ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:someValuesFrom ns1:EMMO_f0b8bace_151e_4f54_8129_c180fd83ae44 ],
@@ -681,20 +704,20 @@ Given by its mean and standard deviation of a lognormal distribution"""@en .
     :EMMO_405ae501-8898-59c0-b2db-0afa09d561f9 "https://en.wikipedia.org/wiki/Crystallite"^^rdf:PlainLiteral ;
     :EMMO_4d45da04-cf90-5d4a-bc11-f76fbd5b5036 "https://www.wikidata.org/wiki/Q899604"^^rdf:PlainLiteral ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass ns1:EMMO_7efd64d1_05a1_49cd_a7f0_783ca050d4f3 ;
+            owl:onClass ns1:EMMO_c1c8ac3c_8a1c_4777_8e0b_14c1f9f9b0c6 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3 ;
+            owl:onClass [ a owl:Class ;
+                    owl:unionOf ( :EMMO_4f709756-86ee-5307-880a-696d08ae9732 :EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d ) ] ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass ns1:EMMO_c1c8ac3c_8a1c_4777_8e0b_14c1f9f9b0c6 ;
+            owl:onClass :EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass [ a owl:Class ;
-                    owl:unionOf ( :EMMO_4f709756-86ee-5307-880a-696d08ae9732 :EMMO_5408b3d3-4971-564b-a34c-53e4e3c3f44d ) ] ;
+            owl:onClass ns1:EMMO_7efd64d1_05a1_49cd_a7f0_783ca050d4f3 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         ns1:EMMO_0bb3b434_73aa_428f_b4e8_2a2468648e19 ;
@@ -773,6 +796,10 @@ Ha = 2 Ku/Js"""@en .
 
 :EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2 a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_329e0b77-853d-5615-8df9-9bee0fd1189e ;
+            owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ],
+        [ a owl:Restriction ;
             owl:onClass :EMMO_572b0885-bd40-51ad-8520-d5477c6b9990 ;
             owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
@@ -780,10 +807,6 @@ Ha = 2 Ku/Js"""@en .
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass :EMMO_5394673b-027e-5afc-bc6f-f72df5ed40a1 ;
             owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ],
-        [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_329e0b77-853d-5615-8df9-9bee0fd1189e ;
-            owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ],
         ns1:EMMO_4207e895_8b83_4318_996a_72cfb32acd94 ;
     skos:prefLabel "GranularMicrostructure"@en ;
     ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "The granular structure of a magnetic materials"@en .
@@ -833,6 +856,14 @@ for a particular value of B.
 The maximum energy product is considered to be the best single index of quality of a permanent magnet material.
 It is twice the energy stored in the stray field of the magnet of optimal shape."""@en .
 
+:EMMO_e838288f-b0b4-5bcb-9889-06b2a10d3ccf a owl:Class ;
+    rdfs:subClassOf [ a owl:Restriction ;
+            owl:hasValue "T0 L+2 M-1 I+1 Θ0 N0 J0"^^xsd:string ;
+            owl:onProperty ns1:EMMO_19d925d0_2cf1_40e5_a391_1a99d68409c9 ],
+        ns1:EMMO_b081b346_7279_46ef_9a3d_2c088fcd79f4 ;
+    skos:prefLabel "AmpereSquareMetrePerKilogram"@en ;
+    ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "Unit of the magnetic moment per unit mass: Am²/kg"@en .
+
 :EMMO_eac1f731-95b1-5f31-ab94-2615535ea223 a owl:Class ;
     rdfs:subClassOf :EMMO_6d90a9fe-5ff3-563b-b33b-ae5a4e1a88d8 ;
     skos:prefLabel "InducedMagneticAnisotropy"@en ;
@@ -865,35 +896,35 @@ It is twice the energy stored in the stray field of the magnet of optimal shape.
     :EMMO_405ae501-8898-59c0-b2db-0afa09d561f9 "https://en.wikipedia.org/wiki/Crystal_structure"^^rdf:PlainLiteral ;
     :EMMO_4d45da04-cf90-5d4a-bc11-f76fbd5b5036 "https://www.wikidata.org/wiki/Q895901"^^rdf:PlainLiteral ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass :EMMO_2ca16b3d-f83e-583c-8292-beb6473ea021 ;
+            owl:onClass :EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_b2a130c3-9688-5358-94ca-f226b85b3009 ;
+            owl:onClass :EMMO_2ca16b3d-f83e-583c-8292-beb6473ea021 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_a205766b-7c02-5c56-90e5-96c553c316c8 ;
+            owl:onClass :EMMO_a1f03bbf-c503-5759-9a26-2562527c0db2 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_5d5fbcc0-2738-5cb8-9157-a0fbe50eebb6 ;
+            owl:onClass :EMMO_ef314f95-f3b5-5cb7-ac56-7bfc54f0d955 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_9977edfa-2b42-55e4-bea0-f39fadca7126 ;
+            owl:onClass :EMMO_a205766b-7c02-5c56-90e5-96c553c316c8 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_a1f03bbf-c503-5759-9a26-2562527c0db2 ;
+            owl:onClass :EMMO_9977edfa-2b42-55e4-bea0-f39fadca7126 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_ef314f95-f3b5-5cb7-ac56-7bfc54f0d955 ;
+            owl:onClass :EMMO_5d5fbcc0-2738-5cb8-9157-a0fbe50eebb6 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_2b7f8b13-d0c3-590c-9851-ca89ce5b7395 ;
+            owl:onClass :EMMO_b2a130c3-9688-5358-94ca-f226b85b3009 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         ns1:EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba ;
@@ -938,21 +969,21 @@ and the easy direction of magnetization."""@en .
 
 :EMMO_75b995e0-2bac-5812-a7f6-f8c1731d1d5c a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass :EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3 ;
+            owl:onClass :EMMO_ada88738-c901-5d83-884b-5f84d27ce527 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_ada88738-c901-5d83-884b-5f84d27ce527 ;
+            owl:onClass :EMMO_2c96e798-57dc-5c12-ad10-f3ec261549d3 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
-        [ a owl:Restriction ;
-            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass :EMMO_b0f0e57e-464d-562f-80ec-b216c92d5e88 ;
             owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ],
+        [ a owl:Restriction ;
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         ns1:EMMO_f1025834_0cd2_42a1_bfeb_13bec41c8655 ;
     skos:prefLabel "GranularStructure"@en ;
     ns1:EMMO_967080e5_2f42_4eb2_a3a9_c58143e835f9 "Ensemble of grains of 1 or more grains"@en .
@@ -1002,16 +1033,16 @@ The coercivity on M(H') loop, where H' is the external field."""@en .
     :EMMO_eb748e96-0aee-5b55-b6be-56b8c6bdaed6 "https://www.electropedia.org/iev/iev.nsf/display?openform&ievref=151-14-06"^^rdf:PlainLiteral ;
     rdfs:subClassOf [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
-            owl:onClass :EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc ;
-            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
-        [ a owl:Restriction ;
             owl:onClass :EMMO_cf5261fe-bdab-5c7b-b6a8-f9a313687bc2 ;
-            owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ;
-            owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
+            owl:onProperty ns1:EMMO_dc57d998_23db_4d8e_b2cd_f346b195b846 ],
         [ a owl:Restriction ;
             owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
             owl:onClass ns1:EMMO_dd4b7d81_28a9_4801_8831_4cbab217e362 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
+        [ a owl:Restriction ;
+            owl:minQualifiedCardinality "0"^^xsd:nonNegativeInteger ;
+            owl:onClass :EMMO_38684bd3-8137-5af1-9c0d-b32bcf58fefc ;
+            owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ],
         [ a owl:Restriction ;
             owl:onClass :EMMO_8a0c8d0a-3dc7-5f3f-ab20-24b38d188827 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
@@ -1061,11 +1092,11 @@ The principal components of the diagonal demagnetizing tensor form the demagneti
 
 :EMMO_b7ebd85f-36aa-540a-b8a9-e2c1094f27f1 a owl:Class ;
     rdfs:subClassOf [ a owl:Restriction ;
-            owl:onClass :EMMO_0213900b-ab6d-56be-82fb-4db874974de1 ;
+            owl:onClass :EMMO_aa999d91-076f-512a-85a0-c2f751c083b1 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         [ a owl:Restriction ;
-            owl:onClass :EMMO_aa999d91-076f-512a-85a0-c2f751c083b1 ;
+            owl:onClass :EMMO_0213900b-ab6d-56be-82fb-4db874974de1 ;
             owl:onProperty ns1:EMMO_e1097637_70d2_4895_973f_2396f04fa204 ;
             owl:qualifiedCardinality "1"^^xsd:nonNegativeInteger ],
         ns1:EMMO_b7bcff25_ffc3_474e_9ab5_01b1664bd4ba ;
diff --git a/src/build_onto.py b/src/build_onto.py
index 190957e..d526566 100644
--- a/src/build_onto.py
+++ b/src/build_onto.py
@@ -181,8 +181,26 @@ class LineEnergy(emmo.PhysicalQuantity):
 
     ## magnetization
 
+    emmo.Magnetization.altLabel = en("VolumeMagnetization")
+    
+    class AmpereSquareMetrePerKilogram(emmo.MeasurementUnit):
+        """Unit of the magnetic moment per unit mass: Am²/kg"""
+        
+        prefLabel = en("AmpereSquareMetrePerKilogram")
+        is_a = [
+            emmo.hasDimensionString.value("T0 L+2 M-1 I+1 Θ0 N0 J0")
+        ]
+
+    class MagneticMomementPerUnitMass(emmo.ElectromagneticQuantity):
+        """Magnetic moment per unit mass, sigma"""
+        
+        comment = en("The magnetization is obtained by multiplying sigma with the density")
+        prefLabel = en("MagneticMomementPerUnitMass")
+        altLabel = pl("sigma, MassMagnetization, SpecificMagneticMoment")
+        is_a = [emmo.hasMeasurementUnit.some(AmpereSquareMetrePerKilogram)]
+
     class SpontaneousMagnetization(emmo.ElectromagneticQuantity):
-        """The spontaneous magnetization, Ms, of a ferromagnet is the result of alignment of the magnetic moments of  individual atoms. Ms exists within a domain of a ferromagnet."""
+        """The spontaneous magnetization, Ms, of a ferromagnet is the result of alignment of the magnetic moments of individual atoms.. Ms exists within a domain of a ferromagnet."""
 
         prefLabel = en("SpontaneousMagnetization")
         altLabel = pl("Ms")
@@ -738,6 +756,15 @@ class InternalSusceptibility(emmo.MagneticSusceptibility):
         altLabel = en("chi")
         wikidataReference = pl("https://www.wikidata.org/wiki/Q691463")
 
+    class MassSusceptibility(emmo.ElectromagneticQuantity):
+        """Ratio of the change of the magnetic moment per unit mass and the internal field: sigma = chi_m H"""
+
+        comment = en("magnetic susceptibility per mass density")
+        prefLabel = en("MassSusceptibility")
+        altLabel = en("chi_m")
+        wikidataReference = pl("https://www.wikidata.org/wiki/Q104655916")
+        is_a = [emmo.hasMeasurementUnit.some(emmo.CubicMetrePerKilogram)]
+
     class AbsolutePermeability(emmo.ElectromagneticQuantity):
         """Ratio of the change of magnetic flux and the internal field: B = mu H"""
 
@@ -871,7 +898,7 @@ class Magnet(emmo.FunctionallyDefinedMaterial):
         is_a = [
             emmo.hasProperty.min(0, emmo.MaterialsProcessing),
             emmo.hasProperty.min(0, emmo.WorkpieceForming),
-            emmo.hasSpatialPart.exactly(1, GranularMicrostructure),
+            emmo.hasSpatialPart.min(0, GranularMicrostructure),
             emmo.hasProperty.exactly(1, ExtrinsicMagneticProperties),
             emmo.hasProperty.min(0, XrayDiffractionData),
         ]