What exactly is the amplitude of an interaction?

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SUMMARY

The discussion centers on the concept of "probability amplitude" in quantum mechanics, particularly as it relates to particle interactions analyzed through Feynman diagrams. The amplitude, denoted as ##\mathcal M##, is crucial for calculating probabilities of interactions, specifically in scattering and decay processes. To derive a probability density, one multiplies the amplitude by its complex conjugate, similar to the calculation of position probability density in standard quantum mechanics. Understanding these concepts requires a solid foundation in quantum mechanics, as advanced texts like Griffiths' may be challenging without prior knowledge.

PREREQUISITES
  • Understanding of quantum mechanics principles, including the Schrödinger equation.
  • Familiarity with Feynman diagrams and their role in particle physics.
  • Knowledge of complex numbers and their conjugates.
  • Basic concepts of scattering and decay processes in quantum field theory (QFT).
NEXT STEPS
  • Study the derivation and implications of probability amplitudes in quantum mechanics.
  • Learn about Feynman diagrams and their applications in calculating scattering cross sections.
  • Explore quantum field theory (QFT) to understand decay widths and related observables.
  • Review foundational quantum mechanics texts to solidify understanding before tackling advanced materials like Griffiths.
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying quantum mechanics and particle physics, as well as educators seeking to clarify the concept of probability amplitudes in their teaching.

Natchanon
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I've been reading Griffths' intro to elementary particles and I encountered this symbol that looks similar to "M" called amplitude, which can be calculated by analyzing the Feynman diagram of an interaction. What exactly is it? When I hear amplitude I imagine waves, but not sure what this one's supposed to mean.
 
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This is the "probability amplitude". You multiply it by its complex conjugate in order to get a type of probability density for the interaction, similarly to the way in ordinary QM the position probability density ##P(\vec x) = |\psi(\vec x)|^2 = \psi^*(\vec x)\psi(\vec x)##.
 
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If you have not seen a quantum mechanical amplitude, it is likely that Griffiths is too advanced for you at the moment. I would suggest backing off to a book on QM, and when you have that down, return to Griffiths,
 
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Vanadium 50 said:
If you have not seen a quantum mechanical amplitude, it is likely that Griffiths is to advanced for you at the moment. I would suggest backing off to a book on QM, and when you have that down, return to Griffiths,
I have read his book intro to quantum mechanics and have taken an intro to QM class. I know about Schrödinger eq and how to calculate probability from it.
 
jtbell said:
This is the "probability amplitude". You multiply it by its complex conjugate in order to get a type of probability density for the interaction, similarly to the way in ordinary QM the position probability density ##P(\vec x) = |\psi(\vec x)|^2 = \psi^*(\vec x)\psi(\vec x)##.
So intergral of|M|^2 is the prob that particular interaction will occur?
 
Natchanon said:
So intergral of|M|^2 is the prob that particular interaction will occur?

Not quite. In particle physics there are two kind of processes: scattering and decays. There are two famous observables that you can calculate with QFT: cross section for the first and decay width for the second.

For both you need ## | \mathcal M | ^ 2 ##, but also some kinematics of the process.

## \mathcal M ## represents somehow the probability, but it is not as direct as in QM.
 
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