Step 1: The work done by the accelerating field equals the kinetic energy: \(qV = \tfrac{1}{2}mv^2\), so the speed is \(v = \sqrt{2qV/m}\).
Step 2: Momentum is \(p = mv = \sqrt{2mqV}\), and wavelength is \(\lambda = h/p\). Since \(h\), \(m\) and \(q\) are fixed, only \(V\) changes, giving \(\lambda \propto V^{-1/2}\).
Step 3: Write the ratio directly. Quadrupling \(V\) multiplies \(\sqrt{V}\) by \(\sqrt{4}=2\), and because \(\lambda\) sits in the denominator, \(\lambda\) is divided by 2.
Step 4: Hence the wavelength becomes half of the original value.
\[\boxed{\lambda' = \frac{\lambda}{2}}\]