Concept:
According to de Broglie's hypothesis,
\[
\lambda=\frac{h}{p},
\]
where \(h\) is Planck's constant and \(p\) is the momentum of the particle.
For a non-relativistic particle,
\[
K=\frac{p^2}{2m}.
\]
Therefore,
\[
p=\sqrt{2mK}.
\]
Substituting into the de Broglie relation,
\[
\lambda=\frac{h}{\sqrt{2mK}}.
\]
Hence,
\[
\lambda\propto\frac{1}{\sqrt{K}}.
\]
Step 1: Write the relation between wavelength and kinetic energy.
Since
\[
\lambda\propto\frac{1}{\sqrt{K}},
\]
we can write
\[
\frac{\lambda_2}{\lambda_1}
=
\sqrt{\frac{K_1}{K_2}}.
\]
Step 2: Use the given information.
The final kinetic energy is four times the initial kinetic energy.
Therefore,
\[
K_2=4K_1.
\]
Substituting,
\[
\frac{\lambda_2}{\lambda_1}
=
\sqrt{\frac{K_1}{4K_1}}.
\]
\[
\frac{\lambda_2}{\lambda_1}
=
\sqrt{\frac{1}{4}}.
\]
\[
\frac{\lambda_2}{\lambda_1}
=
\frac{1}{2}.
\]
Thus,
\[
\lambda_2=\frac{\lambda_1}{2}.
\]
Step 3: Determine the percentage decrease.
Initial wavelength
\[
=\lambda_1.
\]
Final wavelength
\[
=\frac{\lambda_1}{2}.
\]
Decrease
\[
=\lambda_1-\frac{\lambda_1}{2}
=\frac{\lambda_1}{2}.
\]
Percentage decrease
\[
=
\frac{\frac{\lambda_1}{2}}{\lambda_1}\times100
=
50\%.
\]
Step 4: Write the final answer.
The de Broglie wavelength becomes half of its original value.
Hence, it decreases by
\[
50\%.
\]
Therefore,
\[
\boxed{\text{(D)}}
\]
is the correct answer.