Antimatter and bubble chambers?

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SUMMARY

This discussion focuses on the detection of antiparticles, specifically positrons, in bubble chambers made of ordinary matter. It explains that positrons interact with the chamber gas by ionizing atoms, emitting photons along their tracks, rather than annihilating immediately upon collision. The conversation highlights the significance of the range of Coulomb interaction, which is much greater than the range for annihilation, allowing positrons to undergo multiple collisions before annihilation occurs. Additionally, the discussion touches on the concept of impact parameters and the formation of positronium at low energies, which complicates the annihilation process.

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  • Understanding of bubble chamber physics
  • Knowledge of particle-antiparticle interactions
  • Familiarity with ionization processes in gases
  • Basic concepts of quantum mechanics, including cross-sections and impact parameters
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  • Research the principles of bubble chamber operation and particle detection
  • Study the physics of positronium and its formation
  • Explore the concept of cross-sections in particle physics
  • Investigate the role of impact parameters in collision processes
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Physicists, students of particle physics, and anyone interested in the behavior of antiparticles in experimental setups will benefit from this 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 e^{-b.k}, 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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