Electron-Positron production by photon

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Discussion Overview

The discussion centers around the production of electron-positron pairs from photons, specifically addressing the conditions under which this can occur and the conservation laws involved. Participants explore theoretical aspects, practical applications, and the necessary interactions for pair production, with a focus on energy and momentum conservation.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • Some participants question the concept of a "center of mass" for a photon, noting that photons have zero mass and cannot decay into an electron-positron pair without violating conservation laws.
  • Others clarify that pair production requires the presence of another massive charged particle, typically an atomic nucleus, to conserve energy and momentum, and provide the reaction equation for this process.
  • Participants discuss the practical aspects of pair production, mentioning that high-energy photons interacting with materials of high atomic number, such as beryllium or tungsten, are necessary for effective pair production.
  • Some contributions highlight the rarity of direct electron-positron pair production from photon collisions compared to indirect processes involving W bosons.
  • There is a proposal regarding the possibility of pair production from a photon interacting with a massive neutral particle, such as a neutron, with conditions noted for energy ranges.

Areas of Agreement / Disagreement

Participants generally agree that an isolated photon cannot decay into an electron-positron pair due to conservation laws. However, there is no consensus on the specifics of pair production involving other particles, as various models and conditions are discussed.

Contextual Notes

Limitations include the dependence on specific energy ranges and the requirement for additional particles in the interaction for pair production to occur. The discussion also reflects uncertainty regarding the conditions under which pair production can happen with different types of particles.

Silviu
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Hello! I am a bit confused about the decay of a photon into a electron-positron pair. In the center of mass of the photon, isn't this decay violating the energy conservation?
 
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What do you mean by "center of mass of the photon". First of all there's no center of mass, because the photon mass is 0. There's also no center-momentum-frame, because the photon mass is 0, i.e., you can never find a reference frame, where the photon is at rest. As you correctly noted a photon cannot decay to an electron-positron pair, because you cannot fulfill energy-momentum conservation and the on-shell conditions for the photon and the particles simultaneously. So there is no photon decay.
 
Silviu said:
Hello! I am a bit confused about the decay of a photon into a electron-positron pair. In the center of mass of the photon, isn't this decay violating the energy conservation?
As vanhees points out, there is no center of mass frame for a photon - that would be a frame in which the momentum of the photon is zero, and of course there is no such thing.

However, you are on to something here. An isolated photon cannot decay into an electron/positron pair, because there's no way that interaction can conserve both energy and momentum. (An easy way to see this is to think about how the interaction looks in the center of mass frame of the electron and positron after the collision).

Instead, pair production requires the involvement of some other massive charged particle, typically some nearby atomic nucleus. The reaction is properly written as ##\gamma+Z\rightarrow{Z}+e^++e^-## where Z is the other particle; its energy and momentum change in the interaction.
 
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Silviu said:
Hello! I am a bit confused about the decay of a photon into a electron-positron pair. In the center of mass of the photon, isn't this decay violating the energy conservation?

To add to what have been mentioned already in the replies you received, we make e-p pair production by shooting high-energy photons into a material with high atomic number, such as Be. There is a reason for that, and that has been given in the two responses above.

Zz.
 
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ZapperZ said:
by shooting high-energy photons into a material with high atomic number, such as Be
Beryllium has atomic number 4. The only solid target with an even lower number would be lithium, but that is too reactive (chemically) to be practical: Be is as low as you can get.
High atomic numbers would be lead (82) or tungsten (74). You need more material with lighter elements, but the produced electrons/positrons pass through the material easier as well, so low atomic numbers can be favorable.
 
mfb said:
Beryllium has atomic number 4. The only solid target with an even lower number would be lithium, but that is too reactive (chemically) to be practical: Be is as low as you can get.
High atomic numbers would be lead (82) or tungsten (74). You need more material with lighter elements, but the produced electrons/positrons pass through the material easier as well, so low atomic numbers can be favorable.

Sorry, I should have said tungsten. I had Be in my head because I've been shopping around for a Be window for one of our viewports.

Zz.
 
stoomart said:
Positrons and electrons (also neutrinos/antineutrinos) are released from the decay of W bosons after photon collisions.
Technically true, but that is an incredibly rare process. Direct electron and pair production from photon collisions is a very rare process already, but that is much more frequent than the indirect process via W boson production. Note the "collision" part, it doesn't happen with single photons as OP asked about.
 
mfb said:
Technically true, but that is an incredibly rare process. Direct electron and pair production from photon collisions is a very rare process already, but that is much more frequent than the indirect process via W boson production. Note the "collision" part, it doesn't happen with single photons as OP asked about.
Ahh thanks, didnt notice the OP was about a single photon.
 
  • #10
Nugatory said:
However, you are on to something here. An isolated photon cannot decay into an electron/positron pair, because there's no way that interaction can conserve both energy and momentum. (An easy way to see this is to think about how the interaction looks in the center of mass frame of the electron and positron after the collision).
And neither can two or more photons traveling in exact same direction. Nor a photon and another massless particle traveling in exact same direction.
Nugatory said:
Instead, pair production requires the involvement of some other massive charged particle, typically some nearby atomic nucleus. The reaction is properly written as ##\gamma+Z\rightarrow{Z}+e^++e^-## where Z is the other particle; its energy and momentum change in the interaction.

Obviously production of a pair from a photon and a massless chargeless photon traveling in a different direction must be possible because that´s time reversal of annihilation.
Is it possible to produce a pair from a photon and a massive neutral particle, such as neutron?
 
  • #11
snorkack said:
Is it possible to produce a pair from a photon and a massive neutral particle, such as neutron?
Neutrons have charged quarks inside. It is very unlikely in the MeV range, but becomes similar (within a factor of 2) to pair production at a proton at high energies. of a few hundred MeV.
 

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