Branch-cut singularity and the multiparticle contribution to the full propagator

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SUMMARY

This discussion centers on the concept of branch-cut singularities in quantum field theory (QFT) as outlined in Chapter 7 of "An Introduction to Quantum Field Theory" by Peskin & Schroeder. A branch-cut singularity represents a discontinuity in the complex logarithm function, which is less severe than a simple pole singularity. Participants emphasize the importance of understanding these singularities in the context of physical quantities and their mathematical representations, particularly regarding the continuum of poles arising from the complex logarithm of negative numbers. The discussion highlights the necessity of mastering complex analysis to fully grasp these concepts.

PREREQUISITES
  • Understanding of complex analysis, particularly the properties of complex logarithms.
  • Familiarity with quantum field theory concepts, specifically the Kallen Lehman spectral representation.
  • Knowledge of singularities in mathematical functions, including branch cuts and poles.
  • Basic understanding of relativistic energy-momentum relations in physics.
NEXT STEPS
  • Study the properties of branch cuts in complex analysis.
  • Learn about the Kallen Lehman spectral representation in quantum field theory.
  • Explore the implications of singularities in physical models, particularly in QFT.
  • Review "An Introduction to Quantum Field Theory" by Peskin & Schroeder, focusing on Chapter 7.
USEFUL FOR

This discussion is beneficial for physicists, mathematicians, and students of quantum field theory seeking to deepen their understanding of complex analysis and its applications in physics, particularly regarding singularities and their implications in theoretical models.

gremezd
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I have been reading Chapter 7 of Peskin & Schroeder about full propagator, the Kallen Lehman spectral representation, and got stuck at the branch cut singularities and at the complex logarithm of negative numbers. I have posted in the Analysis forum (but have not received any answer) the following question:

Does anyone know what a branch-cut singularity is? I have been trying to understand its importance in physics, but I got lost. I would guess that a singularity in physical context should mean that the value of a function should become very big near that singularity. But if we take complex logarithm, we can become big only in two cases, when the argument is either 0 or infinity.
However, people choose the negative part of a real line in a complex plane as a branch cut for a complex logarithm, and say that this branch cut is a weak singulartiy compared to a simple pole. What do they mean by that?

Can anyone comment something about the "weakness of branch-cut singularities" in QFT or overall in physics.
 
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gremezd said:
Does anyone know what a branch-cut singularity is?
From the sound of your question, I'm guessing you haven't looked at the
Wiki page on this subject? I.e.,

http://en.wikipedia.org/wiki/Branch_cut

I have been trying to understand its importance in physics, but I got lost. I would guess that a singularity in physical context should mean that the value of a function should become very big near that singularity.
More generally, "singularity" can mean that the function becomes ill-defined at that point.
In the case of a branch cut, the function ceases to be single-valued there, which is
not quite as nasty as diverging to infinity at a pole singularity.
 
A branch cut is a curve on the complex plane, across which the function is discontinuous.
 
Yes, I have read wikepedia both on a branch point and complex logarithm.
But how do we interpret singulartities: do they constitute the essence of physical quantities or, as you say, they make these physical quantities ill-defined? and have to be got ridden of?

I found it interesting that the logarithm of negative numbers can be thought of as integrating over a continuum of poles. But it's quite difficult for me to put in one place the images of these different but closely related concepts: branch-cut singularity, continuum of poles, complex logarithm of negative numbers, discontinuity of logarithm at the branch cut; and the meanging of this in a physical context..
 
This is why you should learn the math before you try to learn the physics that uses it.
I'd suggest a book/course on complex analysis.

There's no physical significance of any mathematical thing in itself. Its significance is whatever you decided to give it when you created a mathematical model.
 
well well, maybe I can help you out.
branch-cut singularities are continuous singularities, which means, you have endless singularities from one point on which is the branch-CUT. Now two particles start to exist from p^2=(2m)^2 on. If they have additional energy (see equation for relativistic particles: p^2=E^2+m^2) their momentum p increases, and as the energy can increase continuously you have continuous possible values for p. And with that you have continuous values for M forming poles and these are the possible singularities and obviously this will be a continuum. You can actually look at figure 7.2 in Peskin and it'll become all clear...
 

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