Concept:
The de Broglie wavelength of a moving particle is:
\[
\lambda=\frac{h}{p}
\]
where,
\[
\lambda=\text{de Broglie wavelength}
\]
\[
h=\text{Planck's constant}
\]
\[
p=\text{momentum}
\]
For a non-relativistic particle:
\[
K=\frac{p^2}{2m}
\]
So:
\[
p=\sqrt{2mK}
\]
Therefore:
\[
\lambda=\frac{h}{\sqrt{2mK}}
\]
This means:
\[
\lambda\propto \frac{1}{\sqrt{K}}
\]
Step 1: Write the relation between wavelength and kinetic energy.
Since:
\[
\lambda\propto \frac{1}{\sqrt{K}}
\]
If kinetic energy increases, de Broglie wavelength decreases.
Step 2: Let the initial kinetic energy be \(K\).
Initial wavelength:
\[
\lambda=\frac{h}{\sqrt{2mK}}
\]
Now kinetic energy doubles:
\[
K'=2K
\]
Step 3: Find the new wavelength.
New wavelength:
\[
\lambda'=\frac{h}{\sqrt{2mK'}}
\]
Substitute:
\[
K'=2K
\]
\[
\lambda'=\frac{h}{\sqrt{2m(2K)}}
\]
\[
\lambda'=\frac{h}{\sqrt{2}\sqrt{2mK}}
\]
\[
\lambda'=\frac{\lambda}{\sqrt{2}}
\]
Step 4: Find the factor.
So the wavelength changes by the factor:
\[
\frac{1}{\sqrt{2}}
\]
Step 5: Check the options.
Option (A) \(2\) is incorrect because wavelength decreases, not doubles.
Option (B) \(1/2\) is incorrect.
Option (C) \(\sqrt{2}\) is incorrect because wavelength does not increase.
Option (D) \(1/\sqrt{2}\) is correct.
Hence, the correct answer is:
\[
\boxed{(D)\ \frac{1}{\sqrt{2}}}
\]