Step 1: De-Broglie Wavelength Formula
The de-Broglie wavelength \( \lambda \) is calculated using the following equation, which relates it to an object's momentum \( p \):
\[\n\lambda = \frac{h}{p}\n\]
Where:
- \( h \) represents Planck's constant.
- \( p \) is the object's momentum.
- \( p = mv \), where \( m \) is mass and \( v \) is velocity.
Therefore:
\[\n\lambda = \frac{h}{mv}\n\]
Step 2: Speed and Kinetic Energy Changes
The bus's speed is now doubled. If the original speed is \( v \), the new speed is \( 2v \). The kinetic energy \( K \) of the bus is given by:
\[\nK = \frac{1}{2} m v^2\n\]
When the speed doubles, the new kinetic energy \( K' \) becomes:
\[\nK' = \frac{1}{2} m (2v)^2 = 2 \times \frac{1}{2} m v^2 = 2K\n\]
Thus, the new kinetic energy is twice the original value.
Step 3: De-Broglie Wavelength Alteration
Since the de-Broglie wavelength is inversely proportional to momentum \( p \), and momentum is directly proportional to velocity, the new de-Broglie wavelength \( \lambda' \) can be expressed as:
\[\n\lambda' = \frac{h}{m(2v)} = \frac{1}{2} \times \frac{h}{mv} = \frac{\lambda}{2}\n\]
Step 4: Conclusion
The new de-Broglie wavelength \( \lambda' \) is half the initial wavelength \( \lambda \), so:
\[\n\boxed{(C)} \, \frac{\lambda}{2}\n\]