Let \(E_{n} = \dfrac{- 1}{8 \varepsilon_{0}^{2}} \dfrac{m e^{4}}{n^{2} h^{2}}\) be the energy of the \(n^\text{th}\) level of H-atom. If all the H-atoms are in the ground state and radiation of frequency \(\dfrac{\left(\right. E_{2} - E_{1} \left.\right)}{h}\) falls on it, then:
(a) | it will not be absorbed at all. |
(b) | some of the atoms will move to the first excited state. |
(c) | all atoms will be excited to the \(n = 2\) state. |
(d) | no atoms will make a transition to the \(n = 3\) state. |
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