QFT newbie-creation of particle and anti-particle

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SUMMARY

The discussion centers on the creation of particle-antiparticle pairs from the vacuum in relativistic quantum field theory (QFT). It establishes that when the uncertainty in energy exceeds delta E = 2mc², pairs can emerge due to the zero-point energy associated with a confined particle. The critical size of confinement, L, is linked to the Compton wavelength (ħ/mc), where the kinetic energy of the particle reaches its rest mass energy. The energy required for this process is derived from the particle's motion and the constraints imposed by confinement.

PREREQUISITES
  • Understanding of relativistic quantum field theory (QFT)
  • Familiarity with the uncertainty principle in quantum mechanics
  • Knowledge of zero-point energy concepts
  • Comprehension of Compton wavelength and its significance
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  • Explore the implications of the uncertainty principle in quantum mechanics
  • Study the concept of zero-point energy in quantum systems
  • Investigate the role of confinement in particle physics
  • Learn about the Compton wavelength and its applications in QFT
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Physicists, students of quantum mechanics, and researchers interested in particle physics and quantum field theory will benefit from this discussion.

rsaad
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Hi,
I read the following in an online source:
In relativistic settings, momentum and energy are equal so the uncertainty principle, for a particle of mass m which is trapped in a box of size L, becomes delta E>= [itex]\hbar[/itex]c/L. If uncertainty exceeds delta E=2mc^2, we get pairs of particles and anti-particles from the vacuum.

What I do not understand is these pairs created out of nothing? Has this got to do with field folding up and making these new pairs around the particle in the box?
 
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In relativistic settings, momentum and energy are equal
They are not. Do you mean E=pc for ultrarelativistic particles?

If uncertainty exceeds delta E=2mc^2, we get pairs of particles and anti-particles from the vacuum.
Why should we? The "old" particle cannot just release its energy (what is its state afterwards?), and the new particles could be confined to the potential well, too - so they need even more energy.
 
rsaad said:
In relativistic settings, momentum and energy are equal so the uncertainty principle, for a particle of mass m which is trapped in a box of size L, becomes delta E>= [itex]\hbar[/itex]c/L. If uncertainty exceeds delta E=2mc^2, we get pairs of particles and anti-particles from the vacuum.
Never mind the uncertainty principle, it's the zero point energy that's involved here. If you confine a particle to a box of side L, the particle in its ground state has kinetic energy. As you decrease L, this kinetic energy increases. The critical point comes when the kinetic energy approaches the particle's rest mass mc2, and at this point there will be sufficient energy for additional particles of the same type to be created. The value of L at this point is called the Compton wavelength, equal to ħ/mc.

Note there is no need to wonder where this energy came from - it's already present in the particle's motion. And the particle got that energy from whatever squeezed it into the box.
 

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