To solve this problem, we need to understand the relationship between the de Broglie wavelength \(\lambda\) and the kinetic energy \(E\) of a particle.
The de Broglie wavelength \(\lambda\) is given by the formula:
\(\lambda = \frac{h}{p}\)
where \(h\) is Planck's constant and \(p\) is the momentum of the particle.
The momentum \(p\) can also be expressed in terms of kinetic energy \(E\) as:
\(p = \sqrt{2mE}\)
where \(m\) is the mass of the particle.
Substituting the expression for momentum into the de Broglie wavelength formula, we get:
\(\lambda = \frac{h}{\sqrt{2mE}}\)
Now, we need to find what the wavelength becomes when the kinetic energy is \(\frac{E}{4}\).
However, there seems to be an oversight in this step. Let's re-evaluate from the point we substituted kinetic energy:
- Let's re-calculate when substituting from: \(\lambda' = 2 \cdot \lambda\)
Thus, the correct wavelength \(\lambda'\) when the energy is reduced to \(\frac{E}{4}\) is:
\(\lambda' = 2\lambda\)
Therefore, the correct answer is indeed:
\(2\lambda\)