Photon frequency change taking recoil into account

E_rFinally, we can use this expression to solve for the change in frequency of the emitted photon:\Delta f = f_0 - f = \frac{E_r}{h} = \frac{mc^2 + hf - E_{atom}}{h} = \frac{mc^2 + hf - mc^2 - hf_0}{h} = \frac{hf - hf_0}{h} = f - f_0This means that the change in frequency of the emitted photon is equal to
  • #1
Uniquebum
55
1

Homework Statement


Show that if atom's recoil in transition is [itex]\frac{p^2}{2m}[/itex], the emitted photon's frequency changes by a factor of [itex]1-\frac{\Delta E}{2mc^2}.[/itex]


Homework Equations


Recoil momentum [itex]p = \frac{hf}{c}[/itex]
m = mass of the atom
p = momentum of the electron

The Attempt at a Solution


When photon is absorbed
[itex]E_{atom} = mc^2 + E_{\gamma} = mc^2 + hf_0[/itex]

When the photon is emitted
[itex]\Delta E_{atom} = E_{atom} - E_{\gamma(emitted)} - E_r[/itex] where E_r = recoil energy.
Solving that only leads to
[itex]h(f_0 - f_1) = \Delta E_{atom} - mc^2 + \frac{p^2}{2m}[/itex]
Which doesn't look right... So, what am i doing wrong?
 
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  • #2


it is important to carefully analyze and understand the problem before attempting to solve it. In this case, we are given the information that the recoil momentum of an atom in transition is \frac{p^2}{2m}. This means that when a photon is emitted, the atom experiences a recoil momentum equal to \frac{p^2}{2m}. We also know that the recoil momentum of the atom is related to the frequency of the emitted photon by the equation p = \frac{hf}{c}.

To solve for the change in frequency of the emitted photon, we need to consider the energy conservation of the system. When a photon is absorbed by the atom, the energy of the system is given by E_{atom} = mc^2 + E_{\gamma} = mc^2 + hf_0, where f_0 is the frequency of the absorbed photon. When the photon is emitted, the energy of the system is given by E_{atom} - E_{\gamma(emitted)} - E_r, where E_r is the recoil energy of the atom.

Using the equation p = \frac{hf}{c} and the fact that the recoil momentum is \frac{p^2}{2m}, we can write E_r = \frac{p^2}{2m} = \frac{h^2f^2}{2mc^2}. Substituting this into the energy conservation equation, we get:

E_{atom} = mc^2 + hf_0 = mc^2 + hf - \frac{h^2f^2}{2mc^2}

Solving for f, we get:

f = \frac{hf_0}{mc^2 + hf_0 + \frac{h^2f^2}{2mc^2}}

Now, we can use the fact that \frac{p^2}{2m} = \frac{hf}{c} to get an expression for the recoil energy in terms of the frequency:

E_r = \frac{p^2}{2m} = \frac{h^2f^2}{2mc^2} = \frac{h^2}{2mc^2} \left(\frac{hf}{c}\right)^2 = \frac{h^2f^2}{2mc^2}

Substituting this into the energy conservation equation again, we get:

E
 

FAQ: Photon frequency change taking recoil into account

1. How does recoil affect the frequency of a photon?

Recoil is the result of conservation of momentum in a photon-emitting system. When a photon is emitted, the emitting system experiences a recoil in the opposite direction. This recoil can cause a slight change in the frequency of the emitted photon.

2. Can the change in frequency due to recoil be measured?

Yes, the change in frequency due to recoil can be measured using precision spectroscopy techniques. These techniques involve measuring the frequency of the emitted photon before and after the recoil to determine the change in frequency.

3. Is the change in frequency due to recoil significant?

The change in frequency due to recoil is very small and is typically only noticeable in high-precision experiments. In most cases, the change is negligible and can be ignored.

4. Does the mass of the emitting system affect the change in frequency due to recoil?

Yes, the mass of the emitting system does affect the change in frequency due to recoil. A heavier emitting system will experience a larger recoil and therefore a larger change in frequency compared to a lighter emitting system.

5. Can the change in frequency due to recoil be calculated?

Yes, the change in frequency due to recoil can be calculated using the energy and momentum conservation equations. However, this calculation may be complex and is usually only done in theoretical or high-precision experimental settings.

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