Laplace transform of complementary error function using infinite series

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Use infinite series to derive the Laplace transform relation $L\left\{ \operatorname{erfc}\left(\frac{1}{\sqrt{t}}\right)\right\}= \left(\frac{1}{p}\right)e^{-2\sqrt{p}}$, $a>0$

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HINT:

Use:

$$\text{erfc}\left(\frac{1}{\sqrt{t}}\right)=1-\text{erf}\left(\frac{1}{\sqrt{t}}\right)=1-\frac{2}{\sqrt{\pi}}\sum_{n=0}^{\infty}\frac{(-1)^n\left(\frac{1}{\sqrt{t}}\right)^{1+2n}}{(1+2n)n!}$$


So, we get:

$$\mathcal{L}_t\left[\text{erfc}\left(\frac{1}{\sqrt{t}}\right)\right]_{(\text{s})}=$$ $$\int_0^\infty\text{erfc}\left(\frac{1}{\sqrt{t}}\right)e^{-\text{s}t}\space\text{d}t=\int_0^\infty\left[1-\frac{2}{\sqrt{\pi}}\sum_{n=0}^{\infty}\frac{(-1)^n\left(\frac{1}{\sqrt{t}}\right)^{1+2n}}{(1+2n)n!}\right]e^{-\text{s}t}\space\text{d}t$$ $$\int_0^\infty e^{-\text{s}t}\space\text{d}t-\frac{2}{\sqrt{\pi}}\sum_{n=0}^{\infty}\frac{(-1)^n}{(1+2n)n!}\int_0^\infty\left(\frac{1}{\sqrt{t}}\right)^{1+2n}e^{-\text{s}t}\space\text{d}t$$

Now, use:

  • For the left integral ($\Re[\text{s}]>0$): $$\int_0^\infty e^{-\text{s}t}\space\text{d}t=\mathcal{L}_t\left[1\right]_{(\text{s})}=\frac{1}{\text{s}}$$
  • For the right integral ($\Re[\text{s}]>0$): $$\int_0^\infty\left(\frac{1}{\sqrt{t}}\right)^{1+2n}e^{-\text{s}t}\space\text{d}t=\text{s}^{n-\frac{1}{2}}\Gamma\left(\frac{1}{2}-n\right)$$