Compton scattering in a Feynman diagram

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SUMMARY

This discussion centers on the intricacies of Compton scattering as represented in Feynman diagrams. It highlights two scenarios: (a) an electron absorbing a photon and later emitting one, and (b) an electron emitting a photon and then absorbing one. The conversation delves into the implications of virtual particles and the non-measurable time intervals (t1, t2) during these processes, emphasizing that during these intervals, the existence of real photons is questioned. The participants reference "Student Friendly Quantum Field Theory (Second Edition)" by Robert D. Klauber to support their arguments regarding the nature of virtual particles and the distinction between real and virtual entities in quantum mechanics.

PREREQUISITES
  • Understanding of Compton scattering and its significance in quantum electrodynamics.
  • Familiarity with Feynman diagrams and their role in perturbation theory.
  • Knowledge of virtual particles and the concept of on-shell vs. off-shell states.
  • Basic principles of quantum mechanics, particularly regarding particle interactions.
NEXT STEPS
  • Study the mathematical framework of Feynman diagrams in quantum field theory.
  • Explore the concept of virtual particles and their implications in quantum mechanics.
  • Learn about the significance of time intervals in quantum processes, particularly in Compton scattering.
  • Investigate the differences between real and virtual particles in the context of quantum electrodynamics.
USEFUL FOR

Physicists, students of quantum mechanics, and anyone interested in the foundational concepts of quantum field theory and particle interactions will benefit from this discussion.

nomadreid
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Attempting to understand the following: Compton scattering can happen either
(a) an electron could absorb a photon and later emit a photon, or
(b) an electron could emit a photon and later absorb a photon.
OK, the maths works out, but I am trying to get intuition on track. These two are respectively equivalent to (with apologies to those who don't like the expression "virtual"):
(a*)
(t1) a real electron and a real photon are destroyed and a virtual electron is created
(t2) the virtual electron is destroyed and a real photon and a real electron are created
(b*)
(t1) a real electron is destroyed and a virtual electron and a real photon are created,
(t2) the virtual electron and the real photon are destroyed and a real electron is created.

where t1<t2 (moments in time). The fact that we cannot measure the interval (t1,t2) means that we can't really say what goes on during this time interval, so the paradox that
in (a*) during the interval (t1,t2) nothing real exists, and
in (b*) during the interval (t1,t2) two real photons exist
doesn't bother. So far, so good?
There is the side issue as to how the idea of the existence of continuous time jibes with the idea that small intervals of time don't exist as a real entity. I guess "exists" is taken in two different senses here, right?
 
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Feynman diagrams are just pictorial representations of terms in a perturbation series. EM fields interact with the electron field, always. The diagrams for Compton scattering focus on those interactions which contribute to the desired amplitude which is defined by initial and final states. One of those interactions seems out of causal order but none the less exists in the formal series. Perhaps you are reading too much into the pictures? Just a thought.
 
You may have a point that it may be too much to ask to have each term in the perturbation series correspond to some physical process. In any case, I lifted my rendition of (a), (b),(a*), (b*) almost verbatim from page 225 of "Student Friendly Quantum Field Theory (Second Edition): Basic Principles and Quantum Electrodynamics" by Robert D. Klauber. But in this formulation using annihilation and creation operators, I do not see where causation might seem to be violated: the sequence of events seems OK. My main question rather concerns the "black box" nature of the non-measurable interval of time. If this part is indeed not measurable, how can one talk about real photons existing during that time, as we are doing in (b*)? (The secondary question about the possible graininess of time is an old one, and so I suppose there is no resolution to that conundrum until a successful quantum theory of gravity comes along.)
 
nomadreid said:
how can one talk about real photons existing during that time,

Well, I would suggest we can't. Quantum Mechanics plays havoc with words like "exist" when used in household settings. IMO photons don't exist in the same sense that say bullets or macroscopic particles exist. Personally, I'm happy with this world view. Virtual particles "exist" but only as terms in an operator series expansion. At least, that's how I view it FWIW.
 
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Thanks, Paul Coby. That view of virtual particles is sort of what I meant by the conjunction of the two:
nomadreid said:
(with apologies to those who don't like the expression "virtual")
nomadreid said:
"exists" is taken in two different senses
I am not sure, however, where the boundary is for the distinction between real and virtual for:
(a) photons, electrons, quarks etc. and
(b) collections of these
 
"real" and "virtual" I think are technical terms for on and off mass shell. What I was getting at with "exist" is that macroscopic particles have properties that photons don't. One can quickly be lead to false conclusions and arguments if these things are forgotten. Much head scratching and confusion occurs due to this. For example, a bullet fired at two detectors, A and B, hitting one, either hits A and not B or hits B and not A. For photons from the vast majority of light sources, this is easily shown to be false by looking at the correlation between A and B counts. So, photons don't exist in the same way as bullets.
 
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Granted, at least most of the bullet hits A and not B or vice-versa (and we don't notice the parts that don't follow that pattern). The question is whether the boundary is one of quality or of quantity (quantity becoming quality?). That said, I am thus not sure whether one would say that the situation in the time interval (t1,t2) shouldn't as a whole be described as off-shell, so that during this time interval (and, given the continuity of time, the "during" should have a sense) the photons would also be virtual (as part of a virtual situation, i.e., off shell), and only become "real" (in the sense of being part of a real situation obeying the appropriate equations) outside of this time interval.
 
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Well, the intent of the example I gave is to underscore that real on mass shell photons don't have a trajectory before the fact. If they did then the either or clause of the bullet argument would be valid for them and the counts A and B would show an anti-correlation. In real measurements with light, these counts are uncorrelated. The reason bullet counts are correlated is because they have a well defined trajectory and only one. So it's unclear what one is talking about on the internal lines of a Compton scattering event. So, in this sense, does your question have meaning?

Now, all external lines in a Feynman diagram are on mass shell by definition while all internal lines are off mass shell. A single isolated vertex which depicts a particle which spontaneously belching a photon, will integrate to 0 when all lines are external or on mass shell. It has to be this way to conserve energy and momentum.
 
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OK, thanks for your guidance, Paul Coby. I will try to look at the scattering diagrams with these concepts in mind.
 

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