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	<id>https://the-democratika.com/wiki/index.php?action=history&amp;feed=atom&amp;title=Template%3AInfobox_lawrencium</id>
	<title>Template:Infobox lawrencium - Revision history</title>
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	<updated>2026-04-04T15:47:25Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>https://the-democratika.com/wiki/index.php?title=Template:Infobox_lawrencium&amp;diff=4204&amp;oldid=prev</id>
		<title>&gt;Nucleus hydro elemon at 15:45, 31 July 2024</title>
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		<updated>2024-07-31T15:45:33Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Infobox element&lt;br /&gt;
|symbol =Lr&lt;br /&gt;
|Z      =103&lt;br /&gt;
|number =103&lt;br /&gt;
|name   =lawrencium&lt;br /&gt;
|mass number comment=(data not decisive){{efn|name=&amp;quot;most stable isotope&amp;quot;|The most stable isotope of lawrencium cannot be determined based on existing data due to uncertainty that arises from the low number of measurements. The half-life of &amp;lt;sup&amp;gt;266&amp;lt;/sup&amp;gt;Lr corresponding to one [[standard deviation]] is, based on existing data, {{val|11|21|5}} hours,{{NUBASE2020|ref}} whereas that of &amp;lt;sup&amp;gt;264&amp;lt;/sup&amp;gt;Lr is {{val|4.8|2.2|1.3}} hours;&amp;lt;ref name=Mc2022/&amp;gt; these measurements have overlapping [[confidence interval]]s.}}&lt;br /&gt;
|abundance=&lt;br /&gt;
|abundance in earth&amp;#039;s crust=&lt;br /&gt;
|abundance in oceans=&lt;br /&gt;
|abundance in solar system=&lt;br /&gt;
|left=[[nobelium]]&lt;br /&gt;
|right=[[rutherfordium]]&lt;br /&gt;
|above=[[lutetium|Lu]]&lt;br /&gt;
|below=—&lt;br /&gt;
|appearance=silvery &amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&amp;lt;ref name=&amp;quot;emsley&amp;quot;&amp;gt;{{cite book|last=Emsley|first=John|title=Nature&amp;#039;s Building Blocks: An A-Z Guide to the Elements|edition=New|year=2011|publisher=Oxford University Press|location=New York, NY|isbn=978-0-19-960563-7|page=278–279}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|electrons per shell=2, 8, 18, 32, 32, 8, 3&lt;br /&gt;
|phase=solid&lt;br /&gt;
|phase comment=&amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&lt;br /&gt;
|density gpcm3nrt=14.4&lt;br /&gt;
|density gpcm3nrt comment=&amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&amp;lt;ref name=density&amp;gt;{{cite journal |last1=Gyanchandani |first1=Jyoti |last2=Sikka |first2=S. K. |title=Physical properties of the 6 d -series elements from density functional theory: Close similarity to lighter transition metals |journal=Physical Review B |date=10 May 2011 |volume=83 |issue=17 |pages=172101 |doi=10.1103/PhysRevB.83.172101 |bibcode=2011PhRvB..83q2101G }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|crystal structure=hexagonal close-packed&lt;br /&gt;
|crystal structure comment=&amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&amp;lt;ref name=hcp&amp;gt;{{cite journal|doi=10.1103/PhysRevB.84.113104|title=First-principles calculation of the structural stability of 6d transition metals|year=2011|last1=Östlin|first1=A.|last2=Vitos|first2=L.|journal=Physical Review B|volume=84|issue=11|page=113104|bibcode=2011PhRvB..84k3104O }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|electronegativity=1.3&lt;br /&gt;
|electronegativity comment=&amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&amp;lt;ref&amp;gt;{{cite book |last=Brown |first=Geoffrey |date=2012 |title=The Inaccessible Earth: An integrated view to its structure and composition |publisher=Springer Science &amp;amp; Business Media |page=88 |isbn=9789401115162}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|melting point K=1900&lt;br /&gt;
|melting point C=1600&lt;br /&gt;
|melting point F=3000&lt;br /&gt;
|melting point comment=&amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&lt;br /&gt;
|number of ionization energies=3&lt;br /&gt;
|ionization energy 1=479&lt;br /&gt;
|ionization energy 1 ref=&amp;lt;ref name=&amp;quot;Sato&amp;quot;&amp;gt;{{cite journal |last1=Sato |first1=T. K. |last2=Asai |first2=M. |first3=A. |last3=Borschevsky |first4=T. |last4=Stora |first5=N. |last5=Sato |first6=Y. |last6=Kaneya |first7=K. |last7=Tsukada |first8=Ch. E. |last8=Düllman	 |first9=K. |last9=Eberhardt |first10=E. |last10=Eliav |first11=S. |last11=Ichikawa |first12=U. |last12=Kaldor |first13=J. V. |last13=Kratz |first14=S. |last14=Miyashita |first15=Y. |last15=Nagame |first16=K. |last16=Ooe |first17=A. |last17=Osa |first18=D. |last18=Renisch |first19=J. |last19=Runke |first20=M. |last20=Schädel |first21=P. |last21=Thörle-Pospiech |first22=A. |last22=Toyoshima |first23=N. |last23=Trautmann |date=9 April 2015 |title=Measurement of the first ionization potential of lawrencium, element 103 |journal=Nature |volume=520 |issue=7546 |pages=209–11 |doi=10.1038/nature14342 |bibcode = 2015Natur.520..209S |pmid=25855457|s2cid=4384213 |url=http://cds.cern.ch/record/2008656/files/TKSato-Lr-IP_prep_nature.pdf }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|ionization energy 2=1428.0&lt;br /&gt;
|ionization energy 2 comment = &amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&lt;br /&gt;
|ionization energy 3=2219.1&lt;br /&gt;
|ionization energy 3 comment = &amp;#039;&amp;#039;(predicted)&amp;#039;&amp;#039;&lt;br /&gt;
|CAS number=22537-19-5&lt;br /&gt;
|magnetic susceptibility=&lt;br /&gt;
|magnetic susceptibility ref=&lt;br /&gt;
|naming=after [[Ernest Lawrence]]&lt;br /&gt;
|discovered by=[[Lawrence Berkeley National Laboratory]] and [[Joint Institute for Nuclear Research]]&lt;br /&gt;
|discovery date=1961–1971&lt;br /&gt;
|QID=Q1905&lt;br /&gt;
}}&amp;lt;!--&lt;br /&gt;
&lt;br /&gt;
--&amp;gt;&amp;lt;noinclude&amp;gt;&lt;br /&gt;
{{Infobox element/element navigation|symbol=Lr}}&lt;br /&gt;
{{notelist}}&lt;br /&gt;
{{Template reference list}}&lt;br /&gt;
{{documentation|1=Template:Infobox element/doc}}&lt;br /&gt;
&amp;lt;/noinclude&amp;gt;&lt;/div&gt;</summary>
		<author><name>&gt;Nucleus hydro elemon</name></author>
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