$$ u_t=\alpha^2u_{xx}\\ u(x,0)=e^{-x^2} $$
where t>0
i tried to solve it, but not certain
and i got hint
$$
\int_{-\infty}^{\infty} e^{-\xi^2+i\xi x}d\xi=\sqrt\pi e^{-x^2/4}
$$
thanks for your help
$$ u_t=\alpha^2u_{xx}\\ u(x,0)=e^{-x^2} $$
where t>0
i tried to solve it, but not certain
and i got hint
$$
\int_{-\infty}^{\infty} e^{-\xi^2+i\xi x}d\xi=\sqrt\pi e^{-x^2/4}
$$
thanks for your help
Differential equation to be solved: $$\partial_t u(t,x) = \alpha^2 \partial_x^2 u(t,x).$$
Doing a Fourier transform in $x$ gives $$\partial_t \hat{u}(t,\xi) = -\alpha^2 \xi^2 \hat{u}(t,\xi).$$
For fixed $\xi$ this is an ordinary differential equation of order 1 in $t$ with solution: $$\hat{u}(t,\xi) = \hat{u}(0,\xi) e^{-\alpha^2 \xi^2 t}.$$
The initial condition becomes $$\hat{u}(0,\xi) = \mathcal{F}\{ e^{-x^2} \} = \sqrt{\pi}e^{-\xi^2},$$ so we get the solution $$\hat{u}(t,\xi) = \sqrt{\pi} e^{-\xi^2} e^{-\alpha^2 \xi^2 t} = \sqrt{\pi} e^{-(1+\alpha^2t)\xi^2}.$$
Now we take the inverse Fourier transform: $$ u(t,x) = \mathcal{F}^{-1}\{ \sqrt{\pi} e^{-(1+\alpha^2t)\xi^2} \} = \frac{1}{\sqrt{1+\alpha^2 t}} e^{-x^2}. $$