The de-Broglie wavelength is given by:
\[ \lambda_{DB} = \frac{h}{p} = \frac{h}{\sqrt{2mK}}, \]
where \(m\) is the mass, \(K\) is the kinetic energy, and \(p\) is the momentum. Since the particles have the same energy \(K\), the de-Broglie wavelength becomes:
\[ \lambda_{DB} \propto \frac{1}{\sqrt{m}}. \]
Since \(\lambda_{DB} \propto \frac{1}{\sqrt{m}}\), the lighter the mass, the longer the wavelength:
\[ \lambda_e > \lambda_p > \lambda_\alpha. \]
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to: