Do you use QM in Conjunction With QED/QCD?

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Quantum Mechanics (QM) serves as the foundational theory upon which Quantum Electrodynamics (QED) and Quantum Chromodynamics (QCD) are built. QED focuses on the quantum mechanics of the electromagnetic field, while QCD addresses the quantum mechanics of the color field. All standard QM rules apply to both QED and QCD, although the Born interpretation of the wavefunction may become less clear due to non-conservation of particle number in Quantum Field Theory (QFT). In QFT, the field operator is the primary focus, representing a multiparticle theory that describes the creation and destruction of quanta in spacetime.

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  • Familiarity with Quantum Electrodynamics (QED)
  • Knowledge of Quantum Chromodynamics (QCD)
  • Basic concepts of Quantum Field Theory (QFT)
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  • Study the principles of Quantum Field Theory (QFT)
  • Explore the implications of the Born interpretation in QFT
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  • Investigate the differences between single-particle QM and multiparticle theories
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Do you still use QM in conjunction with the other theories? Is QM kind of like the basic theory that the others rely on? (Hopefully those questions make sense)
 
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QED and QCD are specific quantum field theories. As a subject, quantum field theory is a subset of quantum mechanics: quantum field theory is the quantum mechanics of fields. QED is the quantum mechanics of the electromagnetic field. QCD is the quantum mechanics of the color field.
 
Do all the standard QM rules apply to QED and QCD?
 
Yes. But what in particular are you thinking of as "all the standard QM rules"?
 
If you define electrodynamics to be the study of matter with the electromagnetic field (i.e. with photons), then QED is simply a fully quantum-mechanical approach to that study. In that sense, the "standard QM rules" apply since what you're doing is simply applying QM to yet another problem.

One caveat to this discussion is that the Born interpretation of the wavefunction becomes a bit shaky. The reason is that in quantum field theory (QFT), particle number is not necessarily conserved. This is of little concern because what we would normally call a wavefunction function in single-particle QM yields calculable results in QFT for things we actually measure like scattering experiments, etc.
 
Quantum mechanics deals with single particle systems, which have a small number of degrees of freedom (think observables.) For example, a single particle has associated observables x and p. A quantum field is the quantum mechanical version of the classical field, which describes (maybe infinitely) many degrees of freedom. What makes the quantum field quantum is that these observables are quantized. The observables are particles, making quantum field theory a multiparticle theory: the field describes the creation and destruction of quanta as a function of spacetime.

In QFT, the field operator becomes the dynamical quantity of interest, rather than the single particle wavefunction.
 
Awesome, thanks guys.
 

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