$A$ proton accelerated through a potential $V$ has de-Broglie wavelength $\lambda$. Then the de-Broglie wavelength of an $\alpha$-particle,when accelerated through the same potential $V$ is :

  • A
    $\frac{\lambda}{2}$
  • B
    $\frac{\lambda}{\sqrt{2}}$
  • C
    $\frac{\lambda}{2 \sqrt{2}}$
  • D
    $\frac{\lambda}{8}$

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