2. Consider the EM wave mode with wave vector k and frequency f, in a cavity of temperature T. The average number of photons in the mode, in the limit where $k_{B}T \gg hf$, is given by $(k_{B} = \text{Boltzmann constant}, h = \text{Planck constant})$
(A) $\left[\frac{k_B T}{h f}\right]^2$
(B) $\frac{1}{\left[\exp\left(\frac{k_B T}{h f}\right) - 1\right]}$
(C) $\frac{k_B T}{h f}$
(D) $\exp\left(\frac{-hf}{k_B T}\right)$
(E) $\frac{1}{\left[\exp\left(\frac{hf}{k_B T}\right) + 1\right]}$

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