Head-On Collisions of True Point Charges

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SUMMARY

The discussion centers on the head-on collisions of true point charges, specifically electrons and positrons. It clarifies that while these particles are represented by wave packets with finite spatial extent, precise head-on collisions are not necessary for significant interactions. The concept of positronium, a system where a positron replaces the proton in a hydrogen-like atom, is introduced, highlighting its decay via self-annihilation into photons. The interaction between these particles is mediated by vector bosons, such as photons, and the field created by these charges is described by a "Dirac peak" distribution for point-like particles.

PREREQUISITES
  • Understanding of quantum mechanics and wave-particle duality
  • Familiarity with particle physics concepts, including true point charges
  • Knowledge of positronium and its properties
  • Basic grasp of electromagnetic interactions and vector bosons
NEXT STEPS
  • Research the properties and behavior of positronium in quantum mechanics
  • Study the role of vector bosons in particle interactions
  • Explore the Fourier transform in the context of charge distributions
  • Investigate the implications of Dirac peaks in quantum field theory
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Physicists, students of quantum mechanics, and anyone interested in the interactions of fundamental particles and their theoretical implications.

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Since the electron and the positron are indeed true "point charges" then why are the colliders able to make them collide head-on?
 
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As free particles, the electron and positron are not localized; they are represented by wave packets that have finite spatial extent. Furthermore, it is not necessary for them to collide *precisely* head-on for something interesting to happen. Consider the hydrongen-like 'atom' where the proton is replaced by a positron. This system is called positronium, and has been extensively studied. It decays by self-annihilation into photons, but the wavefunctions describing the system are those of a hydrogen atom.
 
The particles interact via another exhanged virtual particle, which is called a vector boson. For instance, the vector boson for electromagnetic interaction is the photon. Classically thinking, one would say that one particle is actually scattered by the field created around the other particle. Now, the shape of this field depends on the distribution of the charges : for pointlike particles, the distribution is called a "Dirac peak". If the electron were a small ball, as for instance is the proton, then the distribution would look like a fuzzy sphere, as it actually does for the proton, but does not (as precisely as we can see) for the electron.

To be more accurate, the potential for the field created by a distribution of charge is given by the Fourier transform of the distribution (in a certain approximation).
 

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