Feynman Diagrams- Not Conserving Momentum?

In summary: They're called "virtual" because they never actually exist. They're just a by-product of the perturbation theory you're using.
  • #1
nhmllr
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I'm reading QED. At first I thought I understood Feynman diagrams, but due to ones like these I'm not so sure anymore. In either of these diagrams, the photon "curves" around in space time. Why would it travel in anything BUT a straight line if nothing is influencing it? I liked to picture these diagrams in my head as billiard balls going around knocking into other ones, keeping momentum conserved. But here, momentum is CLEARLY NOT conserved. If you look at the initial state of (a) even, the electron is traveling slower at first, then speeds up! What's going on here!?
 
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  • #2
Don't picture particles as billiard balls. Feynman diagrams are just convenient pictures to depict calculations. In QM, particles are also waves, so the whole notion of "particles as billiard balls" doesn't make sense at all. Also, you can't get any notion of speed from these diagrams.

Momentum is conserved at every vertex in these diagrams. It is given by the wavenumber of the particles.
 
  • #3
haushofer said:
Don't picture particles as billiard balls. Feynman diagrams are just convenient pictures to depict calculations. In QM, particles are also waves, so the whole notion of "particles as billiard balls" doesn't make sense at all. Also, you can't get any notion of speed from these diagrams.

Momentum is conserved at every vertex in these diagrams. It is given by the wavenumber of the particles.
Wait if the y-axis is time and the x is space, then a line with a greater slope is moving slower- right? Can't you tell speed like that- or am I reading too much into this?
 
  • #4
You're reading too much into this. The only thing meaningful about the diagram is its topology.
 
  • #5
Feynman diagrams are topological graphs. It only matters what points (vertices) are connected by the lines (propagators) and not their shape. When written in momentum space, there isn't even a time direction.
 
  • #6
Dickfore said:
Feynman diagrams are topological graphs. It only matters what points (vertices) are connected by the lines (propagators) and not their shape. When written in momentum space, there isn't even a time direction.

But COULD you make a Feynman diagram with units? And if so, what would be happenig with these loopy photons?
 
  • #7
nhmllr said:
But COULD you make a Feynman diagram with units? And if so, what would be happenig with these loopy photons?

What 'units'?
 
  • #8
nhmllr said:
But COULD you make a Feynman diagram with units? And if so, what would be happenig with these loopy photons?
No. That would imply that you know the exact trajectory of the electron as a point particle. Particles are waves in QM.

These loopy photons are a remnant of the fact that you're doing perturbation theory, and are called "virtual". They never appear in an in- or outstate, as such are never directly measured, and as such cannot be assigned a velocity or definite energy.
 

FAQ: Feynman Diagrams- Not Conserving Momentum?

1. What are Feynman diagrams?

Feynman diagrams are graphical representations of particle interactions in quantum field theory. They were developed by physicist Richard Feynman in the 1940s as a way to visualize and calculate the probability of different particle interactions.

2. How do Feynman diagrams work?

Feynman diagrams use lines and vertices to represent particles and their interactions. The lines represent particles and their movement through time, while the vertices represent interactions between particles. By following the rules of quantum field theory, Feynman diagrams can be used to calculate the probability of different particle interactions.

3. Why is momentum not conserved in some Feynman diagrams?

In classical physics, momentum is always conserved in interactions between particles. However, in quantum mechanics, there is a small but non-zero chance of particles spontaneously appearing and disappearing. These virtual particles can temporarily disrupt the conservation of momentum in Feynman diagrams.

4. How does this violation of momentum conservation affect our understanding of physics?

The violation of momentum conservation in Feynman diagrams is a result of the probabilistic nature of quantum mechanics. It does not contradict the principles of conservation of momentum in classical physics. In fact, Feynman diagrams have been incredibly successful in predicting and explaining the behavior of particles in quantum field theory.

5. Are there any practical applications of Feynman diagrams?

Feynman diagrams have been used to calculate the probability of particle interactions in various fields such as particle physics, nuclear physics, and condensed matter physics. They have also been used in the development of quantum computing and the study of black holes. Additionally, Feynman diagrams have been used in education to help students better understand complex concepts in physics.

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