Step 1: Recall the governing principle.
Diffusion in solids under constant surface concentration conditions is described by Fick’s second law. The general solution gives:
\[
C(x,t) = C_s \, \text{erfc} \left( \frac{x}{2\sqrt{Dt}} \right)
\]
Here, $C_s$ is the surface concentration, $D$ is diffusivity, $x$ is depth, and $t$ is time.
For a fixed concentration at depth $x$, the term $\frac{x}{\sqrt{t}}$ must remain constant.
Step 2: Establish proportionality relation.
Thus:
\[
\frac{x_1}{\sqrt{t_1}} = \frac{x_2}{\sqrt{t_2}} \Rightarrow t_2 = t_1 \left( \frac{x_2}{x_1} \right)^2
\]
Step 3: Substitute known values.
\[
t_1 = 1000 \, s, x_1 = 1 \, \mu m, x_2 = 2 \, \mu m
\]
\[
t_2 = 1000 \times \left( \frac{2}{1} \right)^2
\]
\[
t_2 = 1000 \times 4 = 4000 \, s
\]
Step 4: Interpretation.
This means that to reach the same Boron concentration at twice the depth, the diffusion process requires four times the time, since depth grows with $\sqrt{t}$.
Final Answer:
\[
\boxed{4000 \, \text{seconds}}
\]