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Update Dicke model.md
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Dicke model.md

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@@ -140,15 +140,14 @@ Superradiance might at first seem counterintuitive, but we can understand it fro
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Let's take the example of 2 excitations amongst 4 TLS. The initial delocalised Dicke state looks like:
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$$
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```{=latex}
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\begin{multline}
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\Psi_i =
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\frac{1}{\sqrt{6}} \big(
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|0,+,+,-,-\rangle + |0,+,-,+,-\rangle + |0,+,-,-,+\rangle \\
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+ |0,-,+,+,-\rangle + |0,-,+,-,+\rangle + |0,-,-,+,+\rangle
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\big)
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\end{multline}
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$$
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We can see there are 6 different configurations for the TLS. Each of the 2 excitations in those 6 configurations could transition from $+$ to a $-$ with a release of a single field quanta. That means each of the 6 configurations has 2 emission paths that it could go in order to reach one of 4 configurations in final the state:
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