Step 1: Formula for de-Broglie Wavelength
The de-Broglie wavelength \( \lambda \) is related to the momentum \( p \) of the object by the following equation:
\[
\lambda = \frac{h}{p}
\]
Where:
- \( h \) is Planck's constant,
- \( p \) is the momentum of the object, and
- \( p = mv \) (for an object of mass \( m \) moving with velocity \( v \)).
Thus:
\[
\lambda = \frac{h}{mv}
\]
Step 2: Change in Speed and Kinetic Energy
Now, the bus's speed is doubled. If the initial speed is \( v \), the new speed is \( 2v \). The kinetic energy \( K \) of the bus is given by:
\[
K = \frac{1}{2} m v^2
\]
When the speed is doubled, the new kinetic energy \( K' \) becomes:
\[
K' = \frac{1}{2} m (2v)^2 = 2 \times \frac{1}{2} m v^2 = 2K
\]
Thus, the new kinetic energy is twice the initial value.
Step 3: Change in de-Broglie Wavelength
Since the de-Broglie wavelength depends inversely on the momentum \( p \), and momentum is directly proportional to velocity, we can write the new de-Broglie wavelength \( \lambda' \) as:
\[
\lambda' = \frac{h}{m(2v)} = \frac{1}{2} \times \frac{h}{mv} = \frac{\lambda}{2}
\]
Step 4: Conclusion
The new de-Broglie wavelength \( \lambda' \) is half of the initial wavelength \( \lambda \), so:
\[
\boxed{(C)} \, \frac{\lambda}{2}
\]