The wavelength of a very fast-moving electron $(v \approx c)$ is:

  • A
    $\lambda = \frac{h}{m_0 v / \sqrt{1 - \frac{v^2}{c^2}}}$
  • B
    $\lambda = \frac{h}{\sqrt{2 m_0 E}}$
  • C
    $\lambda^2 = \frac{h^2}{\sqrt{2 m_0 E}}$
  • D
    $\lambda = \frac{h}{m_0 v}$

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