What is the physical interpretation of n-particle correlation function in QFT?

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Discussion Overview

The discussion revolves around the physical interpretation of n-particle correlation functions in quantum field theory (QFT). Participants explore various aspects of correlation functions, including their roles in scattering processes, decay probabilities, and the relationship to operators and observables in quantum mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants note that correlation functions have different physical interpretations depending on the specific function being discussed.
  • One participant mentions the LSZ formula, which relates certain correlation functions to scattering and decay probabilities.
  • The Källén–Lehmann spectral representation is highlighted as a means to understand the physical spectrum of the theory.
  • The Kubo formula is referenced as a way to describe how one operator changes when perturbed by another operator, linking this to field correlators.
  • A participant interprets the two-point function as the propagation amplitude of a particle, questioning how to interpret n-point correlation functions and mentioning Wick's theorem for breaking them down into sums and products of two-point functions.
  • Another participant reiterates that the LSZ formula is commonly used in introductory QFT courses to relate n-point functions to scattering or decay processes involving multiple particles.
  • It is noted that all operators in the theory can be expressed in terms of fields, indicating that n-point functions appear frequently in various calculations.

Areas of Agreement / Disagreement

Participants express varying interpretations of n-particle correlation functions and their applications, indicating that multiple competing views remain. The discussion does not reach a consensus on a singular interpretation.

Contextual Notes

Participants reference specific formulas and concepts from quantum field theory, but the discussion does not resolve the complexities or assumptions underlying these interpretations.

bengeof
Hi
I would be happy if anyone helped me understand what the physical meaning of n-particle correlation function in QFT is ?
 
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Are you familiar with operators, observables, and matrix elements in introductory quantum mechanics?

The correlation functions have many different physical interpretations depending on which correlation function you're asking about. This is because your physical observables (which are operators) can be built out of quantum fields, so the expectation values, variances, probabilities, and matrix elements of your theory are made out of correlation functions. As some definite examples:

The LSZ formula relates certain correlation functions to scattering and decay probabilities: https://en.wikipedia.org/wiki/LSZ_reduction_formula

The Källén–Lehmann spectral representation of a field tells you about the physical spectrum of the theory by telling you the energy of excitations created by the field: https://en.wikipedia.org/wiki/Källén–Lehmann_spectral_representation

The Kubo formula tells you how one operator changes if you perturb your system by a different operator (since all operators are built out of fields, these are also field correlators): https://en.wikipedia.org/wiki/Kubo_formula
 
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Thank you for your response. Yes my background is QM as done in Griffiths( So yes I have a background of operators, observables and scattering matrix), Classical fields as done in Goldstein and Particle physics as in Griffiths. Griffiths actually works out Feynman rules for QED and QCD.

2 point function is interpreted as propagation amplitude of a particle from x to y, so how does one interpret a n-point correlation function. I know wick's theorem is used to break it down to sums and products of two point functions? isn't that how it works?
 
The usual interpretation seen often in an introductory quantum field theory course is the calculations of particle scattering or decay using the LSZ formula I mentioned above. This formula relates an ("amputated") N-point function to a scattering/decay process involving N particles coming both "in" and "out." For example, let's say you have a theory of scalar particles, call them mesons. If you want the scattering amplitude of two mesons coming in and two mesons coming out, it is related to the 4-point function.

But once again, since all operators in your theory can be written in terms of the fields, and expectation values of operators are then N-point functions, they show up everywhere.
 
Thank you for your response
 

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