In mathematics, the Hahn decomposition theorem, named after the Austrian mathematician Hans Hahn, states that for any measurable space ( X , Σ ) {\displaystyle (X,\Sigma )} and any signed measure μ {\displaystyle \mu } defined on the σ {\displaystyle \sigma } -algebra Σ {\displaystyle \Sigma } , there exist two Σ {\displaystyle \Sigma } -measurable sets, P {\displaystyle P} and N {\displaystyle N} , of X {\displaystyle X} such that:
Moreover, this decomposition is essentially unique, meaning that for any other pair ( P ′ , N ′ ) {\displaystyle (P',N')} of Σ {\displaystyle \Sigma } -measurable subsets of X {\displaystyle X} fulfilling the three conditions above, the symmetric differences P △ P ′ {\displaystyle P\triangle P'} and N △ N ′ {\displaystyle N\triangle N'} are μ {\displaystyle \mu } -null sets in the strong sense that every Σ {\displaystyle \Sigma } -measurable subset of them has zero measure. The pair ( P , N ) {\displaystyle (P,N)} is then called a Hahn decomposition of the signed measure μ {\displaystyle \mu } .