The de Broglie wavelength $(\lambda)$ associated with a photoelectron varies with the frequency $(v)$ of the incident radiation as,[$v_0$ is threshold frequency]:

  • A
    $\lambda \propto \frac{1}{(v - v_0)}$
  • B
    $\lambda \propto \frac{1}{(v - v_0)^{\frac{1}{4}}}$
  • C
    $\lambda \propto \frac{1}{(v - v_0)^{\frac{3}{2}}}$
  • D
    $\lambda \propto \frac{1}{(v - v_0)^{\frac{1}{2}}}$

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The wave nature of an electron was first given by

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