Particle-Antiparticle Pairs: When High Energy Photons Split

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Discussion Overview

The discussion centers on the conditions under which high-energy photons can produce particle-antiparticle pairs, specifically focusing on pair production processes in different contexts, such as interactions with nuclei and photon collisions.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that pair production occurs when the energy of a photon exceeds twice the mass of the particle being produced, specifically mentioning electron-positron pairs requiring energy above 1.02 MeV.
  • Others argue that for pair production to occur, the photon must interact with a nucleus to conserve momentum, or alternatively, two photons can collide to produce pairs, as noted in discussions about conditions post-Big Bang.
  • A participant questions why momentum cannot be transferred to the particle-antiparticle pair itself, leading to further clarification that a massless photon cannot split into two massive particles without a third body to conserve momentum.
  • Another participant elaborates on the necessity of a nucleus or another heavy charged particle in the pair production process, emphasizing the role of momentum conservation in different scenarios.
  • There is a clarification that while a single photon cannot produce a pair due to momentum conservation issues, two photons can collide to create a pair without violating conservation laws.

Areas of Agreement / Disagreement

Participants express differing views on the mechanisms of pair production, particularly regarding the necessity of a nucleus versus the possibility of photon-photon collisions. The discussion remains unresolved with multiple competing perspectives on the conditions required for pair production.

Contextual Notes

Participants highlight the importance of momentum conservation in the context of pair production, noting that the processes discussed depend on specific interactions and conditions that are not universally applicable.

kashiark
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when do high energy photons become a paritcle/antiparticle pair?
 
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it can become when its energy is above twice the particle mass.

e.g. pair production of electron + positron is possible when the photon has energy above 2*m_e = 1022keV
 
malawi_glenn said:
it can become when its energy is above twice the particle mass.

e.g. pair production of electron + positron is possible when the photon has energy above 2*m_e = 1022keV

Your description is somewhat incomplete. In order for pair production to take place the photon has to interact with a nucleus so that momentum conservation will hold. Alternatively if two photons collide (such as just after the big bang) pair production will also be possible.
 
Pair production requires BOTH the photon energy exceeding 1.02 MeV, AND something momentum can be transferred to, like a nucleus. The cross section is proportional to Z2 Ln(E) from 3 MeV to over 1 GeV. (E = hv)
 
why can't the momentum be transferred to to the particle/antiparticle pair? and what is it transferred to when they collide?
 
kashiark said:
why can't the momentum be transferred to to the particle/antiparticle pair? and what is it transferred to when they collide?

photon -> e+ e- violates momentum conservation, as mathman told you.

The photon must 'interact' with a nucleus or other heavy, electrically charged particle, to make pair production possible.

http://en.wikipedia.org/wiki/Pair_production

here is feynman diagram (the process to the left)

http://musr.physics.ubc.ca/~jess/p200/emc2/img48.gif
 
Last edited by a moderator:
what about the photons colliding after the big bang?
 
they can 'collide' with each other, as mathman told you also. Don't you read the answers you've got?
 
"Alternatively if two photons collide (such as just after the big bang) pair production will also be possible."
"The photon must 'interact' with a nucleus or other heavy, electrically charged particle, to make pair production possible."
they seem to contradict each other don't they? i was asking about the physics of the first and i would appreciate it if you would not insult me
 
  • #10
because in post #5 you are referring to post #4 where the "pair production in matter" was discussed by Bob_S.
 
  • #11
i don't understand if they can conserve momentum by colliding why can't they conserve it otherwise without a nucleus?
 
  • #12
you cannot have a massless thing split to two massive things and still conserve momentum. just work it out.

you CAN, on the other hand, have two (massless or massive) things go to two massive things and conserve momentum and energy.

so as to the DIFFERENT processes that you are referring to:

1. photon -> e+ e- : that violates momentum conservation.

2. photon + Nucleus -> e+ e- + nucleus: that is allowed by momentum conservation (think of the nucleus as a "catalyst" that allows the process to occur).

3. photon + photon -> e+ e- : that is also allowed by momentum conservation.

mometum conservation is nothing deep: it's straight out of first-year physics.
 
  • #13
ah ok i get it thanks everyone
 

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