# How is quantum mechanics compatible with the speed of light limit?

Consider a free electron in space. Let us suppose we measure its position to be at point A with a high degree of accuracy at time 0. If I recall my QM correctly, as time passes the wave function spreads out, and there is a small but finite chance of finding it pretty much anywhere in the universe. Suppose it's measured one second later by a different observer more than one light second away and, although extremely unlikely, this observer discovers that electron. I.e. the electron appears to have traversed the intervening distance faster than light speed. What's going on here?

I can think of several, not necessarily contradictory, possibilities:

1. I'm misremembering how wave functions work, and in particular the wave function has zero (not just very small) amplitude beyond the light speed cone.
2. Since we can't control this travel, no information is transmitted and therefore special relativity is preserved (similar to how non-local correlations from EPR type experiments don't transmit information)
3. Although the difference between positions is greater than could have been traversed by the electron traveling at c, had we measured the momentum instead, we would have always found it to be less than $m_e c$ and it's really the instantaneous momentum that special relativity restricts; not the distance divided by time.
4. My question is ill-posed, and somehow meaningless.

Would anyone care to explain how this issue is resolved?

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 This is one reason why we need quantum field theory. – leongz Dec 31 '12 at 19:58 Welcome Elliotte, good question. I don't know the answer to it, I hope someone with better knowledge in QM will be able to help you. I have a small correction for you about the momentum. In special relativity, the momentum is $p=\gamma m v$, where m is the rest mass, $\gamma = \frac{1}{\sqrt{1-(\frac{v}{c})^2}}$, and v is the velocity. As v tends to c, $\gamma$ tends to infinity, so the momentum can actually be much larger than $mc$. – Andrey B Dec 31 '12 at 20:07 Related: physics.stackexchange.com/q/15282/2451 and links therein. – Qmechanic♦ Jan 27 at 18:17

 So, is it correct to say that if one releases an electron at r=0 at t=0, and waits, then the probability of measuring the electron outside the light cone will be zero, but this is due to the field of a positron which cancels out the propagation of electron outside the light cone? Can one then measure a positron anywhere inside the light cone? – Alexey Bobrick Jan 1 at 22:30 Another comment is that one does not need relativistic quantum field theory for this problem. Dirac theory describes a propagating particle-electron (non field) well enough. – Alexey Bobrick Jan 1 at 22:31 Thanks for the question, Elliotte! In my QFT class, we briefly touched on how the antiparticle field cancels out the superluminal effects of the particle field. But what I don't understand is that the particle still can travel faster than the speed of light. Is there no way one can observe only that? I'm sorry if this is a silly question, I've taken just one semester of QFT..Thanks! – user34801 Jan 2 at 7:19 Good questions, and not at all silly! @Alexey Bobrick: You are correct, there is no amplitude to measure an electron outside the light cone. There is also no amplitude to measure a positron inside the lightcone (if you start with an electron state rather than a positron state!). – Michael Brown Jan 2 at 10:59 @user34801: Your question and Alexey's other question are answered by the same discussion: The "electron field" $\psi$ really is the sum of two terms: a term that annihilates an electron (the convention is backwards - blame Heisenberg) and a term that creates a positron. The conjugate field $\bar{\psi}$ does the reverse. (The opposite action on electron vs. positron states makes it an operator with definite electric charge.) Any operator that acts on electron or positron states must be built up out of these combinations to preserve causality. This is the restriction I mentioned before. – Michael Brown Jan 2 at 11:00