Tadpole graph & normal ordering

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Discussion Overview

The discussion revolves around the elimination of the tadpole graph from perturbation expansions in quantum field theory, specifically in the context of normal ordering and its implications for interactions in quantum electrodynamics (QED). Participants explore theoretical proofs and references related to this topic.

Discussion Character

  • Technical explanation, Debate/contested

Main Points Raised

  • One participant inquires about the proof that tadpole graphs are eliminated when normal ordering is applied to the interaction term in quantum field theory.
  • Another participant suggests that the elimination of the tadpole graph should also remove the mass shift associated with it.
  • A reference to Peskin and Schroder's Chapter 4 is provided, indicating that in QED, tadpoles for the photon must vanish due to charge-conjugation symmetry, which implies that the one-point function for the photon is zero.
  • A mathematical expression is presented to support the claim that the loop integral associated with the tadpole graph vanishes, although the reasoning behind this computation is questioned by another participant.

Areas of Agreement / Disagreement

Participants express differing views on the proof of the vanishing of the tadpole graph. While some agree on the implications of charge-conjugation symmetry, there is uncertainty regarding the direct computation that leads to this conclusion.

Contextual Notes

The discussion includes unresolved mathematical steps related to the computation of the loop integral and the assumptions underlying the symmetry arguments. There is a lack of consensus on the method of proving the elimination of the tadpole graph.

QuantumDevil
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It is said that so called tadpole graph gets eliminated from perturbation expansion if the normal-ordered interaction is adopted. How can it be proved? Can anybody provide some links or any other references about this problems?

[tex]L_{int}=-e:\bar{\psi}\gamma_{\mu}\psi A^{\mu}:[/tex]
 
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Here is attachement with this graph
 

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...and this also should remove the mass shift I suppose.
 
See Peskin and Schroder, Chapter 4.

You can see right away that (at least in QED) tadpoles for the photon must vanish, since QED has a charge-conjugation symmetry in which the photon field is odd, so the one-point function for the photon must vanish. You can also see that the diagram you included vanishes since the loop integral explicitly vanishes:

[tex]\int d^4k\frac{{\rm Tr}[\gamma^\mu(k\!\!\!\slash+m)]}{k^2-m^2}= \int d^4k\frac{4k^\mu+0}{k^2-m^2}=0[/tex]

These two statements are, of course, related.
 
How do you know that it is zero by direct computation?
 

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