Antimatter and bubble chambers?

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Discussion Overview

The discussion revolves around the detection of antiparticles, specifically positrons, in bubble chambers made of ordinary matter. Participants explore the mechanisms of ionization and the conditions under which positrons interact with electrons without immediate annihilation, delving into the implications of these interactions in the context of particle physics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants express confusion about how positrons can be detected in a bubble chamber without immediate annihilation upon collision with electrons.
  • It is noted that positrons, being charged particles, ionize atoms in the bubble chamber, leading to the emission of photons along their track.
  • Concerns are raised about the nature of ionization versus annihilation, questioning why annihilation does not occur at the first collision.
  • One participant suggests that the range of Coulomb interaction is greater than the range for annihilation, implying that there is significant distance between electrons and atoms that allows for multiple interactions before annihilation occurs.
  • Another participant mentions the difficulty in finding quantitative information on the parameters affecting the range of annihilation and suggests that the cross-section for electron-positron annihilation may not capture all relevant dynamics, especially at low energies.
  • It is proposed that positrons are less likely to annihilate while moving quickly and that they need to slow down through scattering before annihilation becomes probable.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the mechanisms of ionization versus annihilation, and there are multiple competing views regarding the conditions under which positrons interact with electrons in a bubble chamber.

Contextual Notes

Limitations include the lack of clarity on the quantitative aspects of annihilation range and the dependence on various parameters, which remain unresolved in the discussion.

Aidyan
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I'm confused now... how can be antiparticles be detected in a bubble chamber which is made of ordinary matter? Why does a positron leave its trace interacting with the chamber gas without annihilating immediately?
 
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Aidyan said:
I'm confused now... how can be antiparticles be detected in a bubble chamber which is made of ordinary matter? Why does a positron leave its trace interacting with the chamber gas without annihilating immediately?
Antimatter is charged, and charged particles ionize atoms in the bubble chamber, which leads to emission of photons along the track.

Positrons (and other charged particles) slow down by collisions, mainly with electrons, and because the positron has the rest mass of an electron, the slowing down is more rapid than for heavier particles.
 
Hmmm... I don't feel this answers the question. Why is there any ionization at all and not an immediate annihilation at the first collision? What is observed are several collisons of a positron with many electrons, and yet no annihilation? That doesen't make sense to me.
 
Why should there be immediate annihilation? Or more quantitatively, how "immediate" do you think it should be, and why? (Remember, if it lasts a microsecond, it will travel 1000 feet)
 
Vanadium 50 said:
Why should there be immediate annihilation? Or more quantitatively, how "immediate" do you think it should be, and why? (Remember, if it lasts a microsecond, it will travel 1000 feet)

In this context "immediate" would mean "at the first collision".
 
Aidyan said:
Hmmm... I don't feel this answers the question. Why is there any ionization at all and not an immediate annihilation at the first collision? What is observed are several collisons of a positron with many electrons, and yet no annihilation? That doesen't make sense to me.
The range of coulomb interaction - attraction or repulsion - is much greater than the range for annihilation. There is a lot of 'distance' between electrons and atoms.
 
Astronuc said:
The range of coulomb interaction - attraction or repulsion - is much greater than the range for annihilation. There is a lot of 'distance' between electrons and atoms.

Ok, this makes more sense... but 'googled' and couldn't find a document explaining how it is quantified. Does someone have an idea from what parameters the range of annihilation depends and/or a typical quantitative value?
 
You are right this does seem difficult to google. I thought about just writing down the cross section for e+e- to two photons, but actually I am not sure that that captures everything since at low energies the e+e- pair usually form the bound state positronium before they annihilate. I also seem to recall there is a thing called the "impact parameter", b, which gives the cross-section a dependence which I think is something like [itex]e^{-b.k}[/itex], so that it goes down as the impact is less "head on" and as the momentum goes up. That doesn't give any hint of the scale that matters though. Also I think it is for two approximately plane wave initial states, which is probably not very reasonable if the target electrons are bound in atoms.

But the overall picture is that the positrons are not very likely to annihilate while they are fast-moving, they need to slow down first by scattering off things.
 

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