Concretely, $\smash {\mathord {\sim }^{\mathrm{symm}}_{R}}$ is the symmetric relation on $A$ defined by

\begin{align*} R^{\mathrm{symm}} & \mathrel {\smash {\overset {\mathclap {\scriptscriptstyle \text{def}}}=}}R\cup R^{\dagger }\\ & = \webleft\{ \webleft (a,b\webright )\in A\times A\ \middle |\ \text{we have $a\sim _{R}b$ or $b\sim _{R}a$}\webright\} .\end{align*}

Clear.


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