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Differential EquationsSuperchallengeLaplace Transforms

Laplace Transforms · Superchallenge problem

Let erf⁡(x)=2π∫0xe−w2dw\operatorname{erf}(x) = \dfrac{2}{\sqrt\pi}\displaystyle\int_0^x e^{-w^2}dw. Using the derivative rule and the shift rule for Laplace transforms, evaluate ∫0∞e−terf⁡ ⁣(t)dt\displaystyle\int_0^\infty e^{-t}\operatorname{erf}\!\left(\sqrt{t}\right)dt.