Compton scattering: electron absorbs then emits a photon?

In summary, Compton scattering can be described as a two-particle wavefunction in quantum mechanics. The individual energies of the electron and photon are no longer definite at the time of collision and in the remote future, and are described by a wavefunction that spreads over a wide range of particle energies. The traditional definition of Compton scattering involves two free particles - the photon and the electron - and is not about the photon interacting with an electron bound in an atom. The original experimental observations were based on bound electrons in carbon atoms, but the binding energy of electrons in heavier elements can be significant. The frequency of the scattered photon is reduced due to Doppler shift, as it starts from a moving frame.
  • #1
Physicist
43
0
Hello,

In Compton scattering, does the electron absorbs a photon and then emit another photon with another energy??

I couldn't understand how would the electron absorb a FRACTION of the photon's energy which is forbidden in QM.

Regards
 
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  • #2
Physicist said:
In Compton scattering, does the electron absorbs a photon and then emit another photon with another energy??

I couldn't understand how would the electron absorb a FRACTION of the photon's energy which is forbidden in QM.

Like everywhere else in quantum mechanics, Compton scattering can be described in terms of a wavefunction evolving in time. In a fair approximation, this can be a two-particle wavefunction in this case. Individual energies of the electron and the photon are usually fixed in the remote past. However, these energies are no longer definite at the time of collision and in the remote future (when scattering cross-sections are measured). They are described by the wavefunction which spreads over a wide range of particle energies. So, your description "the electron absorbs a photon and then emits another photon with another energy" is too simplistic.

Eugene.
 
  • #3
Physicist said:
In Compton scattering, does the electron absorbs a photon and then emit another photon with another energy??

The derivation of wavelength shift in Compton scattering uses only the entrance and exit energies and momenta. It does not require a detailed understanding of the interaction. But the Feynman diagrams show an absorption and a re-emission.
 
  • #4
country boy said:
The derivation of wavelength shift in Compton scattering uses only the entrance and exit energies and momenta. It does not require a detailed understanding of the interaction. But the Feynman diagrams show an absorption and a re-emission.

This is true, because the S-matrix formalism of QFT (which uses Feynman diagrams) is a simplified description of reality. In this formalism we care only about entrance and exit states, and don't ask about what happens in the middle. This simplification is a good match for scattering experiments in high energy physics. However, we shouldn't forget that between entrance and exit states the system undergoes some non-trivial time evolution. This time evolution is not accessible by modern experimental techniques, but it may be accessible in the future.

Eugene.
 
  • #5
Aren't you cracking eggs with sledgehammers here? I haven't treated compton scattering using the wavefunction yet but to my knowledge what happens is an electron in an atom absorbs a photon and rises a few energy levels, and then releases a photon of a different energy by moving down one or more energy levels but not to the ground state (which it eventually reaches by emitting more photons).

Is this wrong?
 
  • #6
The electron is ejected from the atom, and the photon is scattered (or re-emitted) with a lower energy (longer wavelength). Other electrons then fall into lower energy levels and they emit photons. The ejected electron is usually absorbed by another atom where it happens to stop after slowing down.
 
  • #7
Just some guy said:
Aren't you cracking eggs with sledgehammers here? I haven't treated compton scattering using the wavefunction yet but to my knowledge what happens is an electron in an atom absorbs a photon and rises a few energy levels, and then releases a photon of a different energy by moving down one or more energy levels but not to the ground state (which it eventually reaches by emitting more photons).

Is this wrong?

As far as I know, the traditional definition of Compton scattering involves two free particles - the photon and the electron. It is not about the photon interacting with an electron bound in an atom. The latter interaction should be treated by very different methods, of course.

Eugene.
 
  • #8
meopemuk said:
As far as I know, the traditional definition of Compton scattering involves two free particles

traditionally, yeah. but a lot of people call many types of electron-photon scattering "compton." For example, some people I know who do NRIX (non-resonant inelastic x-ray scattering) call the scattering off of valence electrons "valence compton." Etc.

Anyways, to get back to what the original post was regarding. The kinematics are pretty easy, but it's the dynamics that are interesting: In a non-relativistic description of the electron there are actually two types of interaction. An interaction whose diagram looks like the standard QED vertex (but is different) where two electron lines and one photon line meet, and an interaction whose diagram looks like two electron lines and two photon lines all meeting at the same place. I believe that it is the latter diagram which gives rise to free electron compton. See, for example:

Eisenberger and Platzman, "compton scattering of x-rays from bound electrons", Phys. Rev. A, vol. 2, p. 415.
 
  • #9
Arthur H. Compton observed the scattering of x-rays from electrons in a carbon target and found scattered x-rays with a longer wavelength than those incident upon the target.

http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/comptint.html

The original experimental observations were based on bound electrons in carbon atoms. The binding energies of those electrons is in the eV range as opposed to keV energies of photons. Therefore one could treat the electrons as essentially free. Compton was apparently looking at X-ray diffraction among other things.

Of course, if an X-ray or gamma-ray scatters off a K or L electron in a much heavier element, then the binding energy is significant.

See also - http://nobelprize.org/nobel_prizes/physics/laureates/1927/index.html
http://nobelprize.org/nobel_prizes/physics/laureates/1927/compton-lecture.html

or http://nobelprize.org/nobel_prizes/physics/laureates/1927/compton-lecture.pdf (the discussion of the Compton effect begins on page 10 of the pdf file)
 
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  • #10
Astronuc said:
as opposed to keV energies of electrons.

You probably wanted to say: as opposed to keV energies of photons.

Eugene.
 
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  • #11
meopemuk said:
You probably wanted to say: as opposed to keV energies of electrons.

Eugene.
Corrected it. Thanks! :redface:
 
  • #12
Physicist said:
Hello,

In Compton scattering, does the electron absorbs a photon and then emit another photon with another energy??

I couldn't understand how would the electron absorb a FRACTION of the photon's energy which is forbidden in QM.

Regards
You could also see things in this (simplistic) way: because of Doppler shift, the frequency of the scattered photon is reduced because it starts from a moving frame (the pushed electron).
A photon's energy infact depends on the ref. frame, that is: the relative speed of source and observer.
 
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  • #13
Well actually, all of the photon is absorbed by the electron. Some of the energy from the photon is used to remove the electron from the atom and its kinetic energy. The rest is released by the electron. Since E = hc/wavelength, lower energy in the released photon changes its wavelength.
 
  • #14
sheepandgoat said:
Well actually, all of the photon is absorbed by the electron. Some of the energy from the photon is used to remove the electron from the atom and its kinetic energy. The rest is released by the electron. Since E = hc/wavelength, lower energy in the released photon changes its wavelength.
Then what [tex]
\Delta \lambda
[/tex] stands for in the Compton's formula?
 

1. What is Compton scattering?

Compton scattering is a physical phenomenon in which a high-energy photon collides with an electron, transferring some of its energy to the electron and causing it to recoil. The electron then emits a lower-energy photon in a random direction.

2. What is the significance of Compton scattering in physics?

Compton scattering provides evidence for the wave-particle duality of light, as it demonstrates the particle-like behavior of photons. It also has important applications in the fields of X-ray and gamma-ray imaging, as well as in understanding the structure of atoms and molecules.

3. How does Compton scattering differ from other forms of scattering?

Unlike other forms of scattering, such as Rayleigh or Thomson scattering, Compton scattering involves a transfer of energy from the incident photon to the electron. This results in a decrease in the wavelength of the scattered photon, known as the Compton shift.

4. What factors affect the amount of energy transferred in Compton scattering?

The amount of energy transferred in Compton scattering depends on the energy of the incident photon, the angle at which it collides with the electron, and the mass and velocity of the electron. Higher-energy photons, larger scattering angles, and lighter or faster-moving electrons result in greater energy transfers.

5. What are some real-world applications of Compton scattering?

Compton scattering has many practical applications, including in medical imaging techniques such as computed tomography (CT) scans and positron emission tomography (PET) scans. It is also used in X-ray diffraction studies to determine the structure of crystals, and in nuclear physics experiments to study the properties of subatomic particles.

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