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In Lawrence Krauss's book "A Universe From Nothing"; page 62 mentions that for a very short period of time, so small it cannot be measured, an electron due to the uncertainty principle can appear to be moving faster than the speed of light; another way to interpret this is that it's moving back in time.

It further proceeds to say that Feynman used this to suggest that what happens was that an electron and a positron were created, the positron will annihilate with the original electron while the new electron will continue on its merry way.

It finally says that this behavior is confirmed by the spectrum of the Hydrogen atom, among other things.

My question is, how does this not violate special relativity? How is it possible to get an electron moving faster than light? And how did we say it's okay to assume that and simply consider it moving back in time?

(Note, I do not have a degree in Physics so please take that into account while explaining the basic idea).

Qmechanic
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Fingolfin
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  • that interpretation is very old-fashioned. Today we don't believe anything of that is true. – AccidentalFourierTransform Nov 23 '16 at 20:30
  • How was it accepted in the first place given that it seems, to a novice like me, that it violates special relativity? And what did we replace it with? – Fingolfin Nov 23 '16 at 20:51
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    They had nothing better as an alternative. "QM is weird", they thought, "and so let's see how far we can take this absurdities without running into inconsistencies". It was a good attitude, because they were trying to explore as many alternatives as they could (and they always compared their predictions to experiments, which most of the time agreed, sometimes with an astonishing accuracy). They replaced it with Quantum Field Theory. – AccidentalFourierTransform Nov 23 '16 at 20:55
  • A big part of Feynman's work was actually about QFT (he got the Nobel price for his work on QED), so I wouldn't say that what the OP is talking about something different than QFT. It's just the language of virtual particles used in perturbation theory. – coconut Nov 24 '16 at 15:48

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In particle physics, the mathematical framework that is currently used is known as quantum field theory. An example of such a theory is quantum electrodynamics, which deals with the interactions between photons and electrons.

When doing calculations in quantum field theory, you find yourself dealing with a lot of (some times very complex) formulas. Feynman found a way to nicely represent this formulas as diagrams. Two examples of Feynman diagrams are:

e^+ gamma -> e^+ gamma photon self

If you are studying a physical process and you want to make predictions about it there's a recipe to do your calculations:

Draw all the Feynman diagrams corresponding to the process in question. Each diagram has an associated mathematical formula. By adding all of them one gets the physical answer.

There are also some rules (known as Feynman rules) that are used draw diagrams. In general, what you have to do is:

For each incoming photon draw a wavy line on the left, for each incoming electron or positron a solid line (the arrow towards the left means a positron and towards the right an electron) and the same for outgoing particles. Then use the Feynman rules to construct an allowed diagram.

We could stop here. Feynman diagrams are just a nice way of representing some complicated formulas. We know how to use them to get experimentally testable answers to questions about the physics of electrons and photons. The results that can be obtained in this way describe nature impressively precisely (as is the case of the Lamb shift, some effect in the hydrogen atom).

However, because every incoming and outgoing line represents a particle, it is tempting to say that the internal lines of the diagram are also particles. Physicist sometimes call them virtual particles, but the concept of virtual particle has very little to do with the one of particle. Notice that a Feynman diagram doesn't even describe a physical process. It's just a way of representing some mathematical formula.

Why do physicist use that name, then? The answer is that when talking about calculations in quantum field theory, it can be used as a useful metaphor. You can talk about diagrams in a natural way as if they were physical processes with time represented as flowing from left to right and with particles colliding, being created, destroyed, etc.

In this metaphor, virtual particles can travel faster than the speed of light, for example. Nevertheless, when you translate this metaphoric language into the actual formulas and add them for all the diagrams, the results are agree with special relativity. The real particles never get to go faster than light.

In the first of the example diagrams above, the internal vertices can be moved so that one is on the left of the other, so in our metaphor one occur before the other. Then we can move them again and make the one that was in the left be now in the right. The internal solid line representing an electron would then change from going forward in time to going backwards. The metaphor plays nicely with this and allows us to see the electron going backwards as a positron (as both are represented by a solid line with an arrow to the left). Again, none of this is real, it is just a nice way of talking about some calculations.

In the second diagram, you can see an example of virtual creation and annihilation of an electron-positron pair from and to a photon. This is just a fancy way of talking about one diagram in the set of the Feynman diagrams describing the propagation of a photon.

So, to summarize and be very clear:

In quantum field theory special relativity is not violated, and it is impossible for any particle (in particular, electrons) to go faster than the speed of light or backward in time.

coconut
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  • Mind blown Thank you! Do you have a good recommendation for a book on QED or QFT? – Fingolfin Nov 24 '16 at 17:36
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    I'm glad it helped! At a popular science level a great book is "QED: The Strange Theory of Light and Matter", an adaptation from some lectures given by Feynman himself. It has all the ideas and it's really enjoyable. I don't know what your background is, but if you want to start getting into the technical stuff (undergraduate level) a good place to start might be "Introduction to Elementary Particles" by Griffiths although is not strictly about QFT. The standard book nowadays for a one-year course in QFT I'd say that is "An Introduction to Quantum Field Theory" by Peskin. – coconut Nov 24 '16 at 17:58