e t → 1 p − 1 e ^ {t} \rightarrow \frac {1}{p - 1} e t → p − 1 1 1 π t → 1 p \frac {1}{\sqrt {\pi t}} \rightarrow \frac {1}{\sqrt {p}} π t 1 → p 1
By multiplication theorem:
1 p − 1 ⋅ 1 p → ∫ 0 t e t − u d u π u = 2 e t π ∫ 0 t e − u d ( u ) = = 2 e t π ∫ 0 t e − v 2 d ( v ) = e t erf ( t ) \begin{array}{l} \frac {1}{p - 1} \cdot \frac {1}{\sqrt {p}} \rightarrow \int_ {0} ^ {t} e ^ {t - u} \frac {d u}{\sqrt {\pi u}} = \frac {2 e ^ {t}}{\sqrt {\pi}} \int_ {0} ^ {t} e ^ {- u} d (\sqrt {u}) = \\ = \frac {2 e ^ {t}}{\sqrt {\pi}} \int_ {0} ^ {t} e ^ {- v ^ {2}} d (v) = e ^ {t} \operatorname {erf} (\sqrt {t}) \\ \end{array} p − 1 1 ⋅ p 1 → ∫ 0 t e t − u π u d u = π 2 e t ∫ 0 t e − u d ( u ) = = π 2 e t ∫ 0 t e − v 2 d ( v ) = e t erf ( t )
By shift theorem:
erf ( t ) → 1 p p + 1 \operatorname {erf} \left(\sqrt {t}\right)\rightarrow \frac {1}{p \sqrt {p + 1}} erf ( t ) → p p + 1 1