Work in progress

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    <j.0:symbol>A_jkN_j</j.0:symbol>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://electron6.phys.utk.edu/qm2/modules/m10/einstein.htm</j.0:informativeReference>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\frac{-dN_j}{dt} = A_jkN_j$, where $-dN_j$ is the number of molecules spontaneously leaving the state j for the state k during a time interval of duration $dt$, $N_j$ is the number of molecules in the state j, and $E_j &gt; E_k$.</j.0:latexDefinition>
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E0L0I0M0H0T0D1"/>
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    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">Given two atomic states of energy $E_j$ and $E_k$.  Let $E_j &gt; E_k$.  Assume the atom is bathed in radiation of energy density $u(w)$.  Transitions between these states can take place in three different ways. Spontaneous, induced/stimulated emission, and induced absorption. $A_jk$ represents the Einstein transition probability for spontaneous emission.</j.1:description>
    <rdfs:comment>Applicable units are those of quantitykind:EinsteinTransitionProbability</rdfs:comment>
    <rdfs:label xml:lang="en">Einstein Transition Probability</rdfs:label>
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  <http://qudt.org/schema/qudt/latexDefinition> "$\\frac{-dN_j}{dt} = A_jkN_j$, where $-dN_j$ is the number of molecules spontaneously leaving the state j for the state k during a time interval of duration $dt$, $N_j$ is the number of molecules in the state j, and $E_j > E_k$."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/symbol> "A_jkN_j" ;
  rdfs:comment "Applicable units are those of quantitykind:EinsteinTransitionProbability" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Einstein Transition Probability"@en ;
.

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    ,"label":"Einstein Transition Probability" 
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