semi-infinite heat equation with Dirichlet BC via Laplace transforms

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I am trying to solve the heat equation for a semi infinite rod with lateral surfaces insulated and $u(x,0)$ = $u_0$ for $x>0$, $u(0,t)=u_1$ for $t>0$, and the $\lim_{t\to\infty} u(x,t)=u_0$.

I think I need to start with:

$$\frac{d^2u}{dx^2}=\frac{1}{\alpha^2}\frac{du}{dt}$$

Then I take Laplace Transform:

$$\frac{d^2U}{ds^2}-\frac{s}{\alpha^2}U=0$$

Can someone help me with the following steps?