Concept:
The de Broglie wavelength of a particle is:
\[
\lambda=\frac{h}{p}
\]
For a non-relativistic particle:
\[
K=\frac{p^2}{2m}
\]
So:
\[
p=\sqrt{2mK}
\]
Therefore:
\[
\lambda=\frac{h}{\sqrt{2mK}}
\]
This gives:
\[
\lambda\propto \frac{1}{\sqrt{K}}
\]
Step 1: Let the initial energy be \(E\).
Initial de Broglie wavelength is:
\[
\lambda
\]
Since:
\[
\lambda\propto \frac{1}{\sqrt{E}}
\]
Step 2: Energy is reduced to half.
New energy:
\[
E'=\frac{E}{2}
\]
New wavelength:
\[
\lambda'\propto \frac{1}{\sqrt{E'}}
\]
\[
\lambda'\propto \frac{1}{\sqrt{E/2}}
\]
\[
\lambda'\propto \frac{\sqrt{2}}{\sqrt{E}}
\]
So:
\[
\lambda'=\sqrt{2}\lambda
\]
Step 3: Find increase in wavelength.
Increase in wavelength:
\[
\Delta\lambda=\lambda'-\lambda
\]
\[
\Delta\lambda=\sqrt{2}\lambda-\lambda
\]
\[
\Delta\lambda=(\sqrt{2}-1)\lambda
\]
Step 4: Find percentage increase.
Percentage increase:
\[
\frac{\Delta\lambda}{\lambda}\times100
\]
\[
=(\sqrt{2}-1)\times100
\]
Using:
\[
\sqrt{2}\approx1.414
\]
\[
=(1.414-1)\times100
\]
\[
=0.414\times100
\]
\[
=41.4\%
\]
Approximately:
\[
41\%
\]
Step 5: Check the options.
Option (A) \(100\%\) is incorrect.
Option (B) \(61\%\) is incorrect.
Option (C) \(34\%\) is incorrect.
Option (D) \(41\%\) is correct.
Hence, the correct answer is:
\[
\boxed{(D)\ 41\%}
\]