Special Case of Compton Scattering

In summary: In principle, no problem. Except that in the scenario described above the electrons are 'stopped' in the observer reference frame - he/she is not moving alongside the beam because the beam has been 'stopped' relative to him/her. The electrons are 'stationary' in a fashion identical to that of loosely bound electrons in an atom - the original target of Compton scattering experiments.In summary, In a collision with billiard balls, you have a problem with the final velocity of a billiard ball being zero. With a photon-billiard ball collision, you have a problem with the photon having the same energy as the electron at rest.
  • #1
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Is there anything special about a Compton scattering event in which the incident photon has the same energy (512 keV) as the electron at rest ?
Was just wondering if there's anything special about the physics of Compton scattering where the incident photon has the same energy (512 keV) as the electron at rest. Then: $$1−cosθ_d=\frac{E_0ΔE}{Ei Er}=\frac{E_0(E_0−Er)}{E_0E_r}=\frac{E_0}{E_r}−1=\frac{λ_r}{λ_0}−1 $$ $$⇒\frac{1}{E_r}\propto -\cos\theta_d$$ $$⇒\lambda_r\propto -\cos\theta_d$$ where ##E_0## and ##\lambda_0## are the energy and (Compton) wavelength of the stationary electron and ##E_r##,##\lambda_r## are the energy and wavelength of the scattered photon.

Might be relevant if the gamma ray laser ever becomes a reality.
 
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  • #3
Suppose the gamma ray laser becomes a reality. Could it be used for imaging purposes and if so then wouldn't the simplified Compton scattering relationships prove useful ? Just speculating admittedly but Compton effect imaging is already 'real' science:

https://www.nature.com/articles/s41598-019-49130-z
 
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  • #4
There's a result which shows that if the scattered photon has energy equal to the rest mass of the electron, then the trajectories of the scattered photon and the electron are at right angles. Scattering angle is given by ##sin\theta=v/c## where v is the post collision velocity of the electron.

As I imagine it, the 'reverse time' version of this collision is an electron (beam of electrons perhaps) colliding with a gamma ray photon (beam of gamma rays) at right angles. The gamma ray photons have energy equal to rest mass of electrons. The electrons are "stopped" (if that is possible ??) and the gamma photons pick up the energy/momentum and are deflected through an angle ##\theta## where ##sin\theta## = v/c and v is the pre-collision velocity of the electron(s).

Does that sound plausible in 'real' time ? I can't quite imagine how a "stopped" electron would behave!
 
  • #5
neilparker62 said:
The electrons are "stopped" (if that is possible ??)

Why is this a problem? For all scatters there is a frame where the outgoing electron is at rest.
 
  • #6
Ok - so per scenario above, you fire beams of electrons and gamma ray photons (512 keV) at right angles to each other. What happens - does the electron 'beam' simply disappear ? One can imagine stationary electrons within the context of being bound to some atom but not suspended in mid air / mid vacuum as it were. Do they just fall to the ground under gravity or what ?

Alternatively if you want to carry out Compton scattering on 'free' rather than 'bound' electrons, is it possible to have 'free but stationary' electrons ? Stationary in the same way as bound electrons are 'stationary' ?
 
  • #8
neilparker62 said:
What happens - does the electron 'beam' simply disappear ?

Why would it? If you see a beam of electrons moving past you at v=non-zero what is the problem with moving along the beam so v=0 relative to you?
 
  • #9
Vanadium 50 said:
Why would it? If you see a beam of electrons moving past you at v=non-zero what is the problem with moving along the beam so v=0 relative to you?
In principle, no problem. Except that in the scenario described above the electrons are 'stopped' in the observer reference frame - he/she is not moving alongside the beam because the beam has been 'stopped' relative to him/her. The electrons are 'stationary' in a fashion identical to that of loosely bound electrons in an atom - the original target of Compton scattering experiments.

From: https://phys.libretexts.org/Bookshelves/Modern_Physics/Book%3A_Spiral_Modern_Physics_(DAlessandris)/4%3A_The_Photon/4.2%3A_Compton_Scattering

Compton scattering refers to the scattering of light off of free electrons. Experimentally, it’s impossible to create a target of completely free electrons. However, if the incident photons have energy much greater than the typical binding energies of electrons to atoms, the electrons will be “knocked off” of the atoms by the photons and act as free particles. Therefore, Compton scattering typically refers to scattering of high energy photons off of atomic targets.
 
  • #10
Let's go step by step.

OK, so you don't have a problem with a stopped electron.
In a collision with billiard balls, do you have a problem with the final velocity of a billiard ball being zero?
What about a photon-billiard ball collision?
 

1. What is Compton scattering?

Compton scattering is a phenomenon in which a photon (typically X-ray or gamma ray) collides with an electron, resulting in the scattering of the photon at a different energy and direction.

2. What makes Compton scattering a special case?

Compton scattering is considered a special case because it involves the interaction between a photon and a free electron, as opposed to other forms of scattering which involve bound electrons.

3. How does Compton scattering contribute to our understanding of quantum mechanics?

Compton scattering provides evidence for the particle nature of light and the wave-particle duality of matter. It also supports the concept of energy quantization in quantum mechanics.

4. What are the applications of Compton scattering?

Compton scattering is used in various fields such as medical imaging, materials science, and astrophysics. It is also used in particle accelerators to measure the energy and momentum of particles.

5. How is Compton scattering related to the Compton wavelength?

The Compton wavelength is a fundamental constant in quantum mechanics that describes the scale at which quantum effects become significant. It is related to Compton scattering because the wavelength of the scattered photon is affected by the Compton wavelength of the electron involved in the interaction.

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