Question 705072

SCQMEDIUM

An atom of mass mm, initially at rest, resonantly absorbs a photon. It makes a transition from the ground state to an excited state and also gets a momentum kick. If the difference between the energies of the ground state and the excited state is Δ\hbar\Delta, the angular frequency of the absorbed photon is closest to

(A)

Δ(1+32Δmc2)\Delta (1 + \frac{3}{2} \frac{\hbar\Delta}{mc^2})

(B)

Δ(1+12Δmc2)\Delta (1 + \frac{1}{2} \frac{\hbar\Delta}{mc^2})

(C)

Δ(1+Δmc2)\Delta (1 + \frac{\hbar\Delta}{mc^2})

(D)

Δ(1+2Δmc2)\Delta (1 + 2 \frac{\hbar\Delta}{mc^2})

Detailed Solution

Conservation of energy: ω=Δ+p22m\hbar\omega = \hbar\Delta + \frac{p^2}{2m}. Conservation of momentum: p=ωcp = \frac{\hbar\omega}{c}. Substituting pp: ω=Δ+(ω/c)22m\hbar\omega = \hbar\Delta + \frac{(\hbar\omega/c)^2}{2m}. Approximating ωΔ\omega \approx \Delta in the second term gives ωΔ+(Δ)22mc2\hbar\omega \approx \hbar\Delta + \frac{(\hbar\Delta)^2}{2mc^2}. Dividing by \hbar: ω=Δ+Δ22mc2=Δ(1+Δ2mc2)\omega = \Delta + \frac{\hbar\Delta^2}{2mc^2} = \Delta(1 + \frac{\hbar\Delta}{2mc^2}).

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