Probability waves - instant infinite extent?

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Discussion Overview

The discussion revolves around the nature of probability waves in quantum mechanics, particularly focusing on the implications of wavefunctions extending to infinity versus being limited by a propagation speed. Participants explore concepts related to local causality, the behavior of wavefunctions, and the implications of superluminal phenomena.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether limiting the propagation speed of a wavefunction to the speed of light would alter its properties, suggesting that particles created at a point would have zero probability of detection outside a sphere expanding at that speed.
  • Another participant clarifies that while the wavefunction can mathematically extend infinitely, real particles are created as wave-packets with a coherence length, which limits their behavior to classical properties outside this length.
  • It is noted that the wavefunction can exist outside the light cone, but this does not imply actual faster-than-light communication, as local causality is preserved in the Heisenberg picture.
  • A participant challenges the assertion that a wavefunction cannot extend infinitely, arguing that an infinite potential would be required to stop it completely, and references the concept of superluminal neutrinos in relation to time tunneling.
  • Another response emphasizes that a particle cannot be described by a pure momentum state due to the Heisenberg uncertainty principle, which leads to localization of the wavefunction within a finite region of space.

Areas of Agreement / Disagreement

Participants express differing views on the nature of wavefunctions and their propagation characteristics. There is no consensus on whether wavefunctions can extend infinitely or the implications of limiting their propagation speed.

Contextual Notes

Participants reference the Heisenberg uncertainty principle and local causality, indicating that the discussion is grounded in complex quantum mechanical principles that may have unresolved assumptions or implications.

ihatelolcats
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Mathematically they are set up so the wave extends instantly to infinity in all directions, right? What would break if you limited the "propagation speed" to c, so if a particle is created at a point in space it would have 0 probability of being detected outside a sphere expanding at c away from that point?
 
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There are two separate issues here.. one is local causality (whether or not information can be transmitted faster than light) and the other is the shape of the wavefunction.

As to the second point, there's a simple answer: it's true that the solution to Schrödinger's equation with no electrostatic potential is a constant wave that extends infinitely; any other function would not be a stationary state and would evolve over time. In reality, particles are created at some point in time with a range of energies, so the wavefunction is initially formed as a wave-packet with a "coherence length". Within this coherence length the particle behaves as a wave and can exhibit interference effects, but outside it behaves as a particle and reproduces classical behaviour. Since this wave-packet is not a stationary solution of the Schrödinger equation it will evolve over time the same way ordinary waves do so in a dispersive medium. Since the coherence length is limited by external "noise" (random fluctuations in the external potential), whether its other particles, or, in a material, defects or impurities, it is impossible to get a single wavefunction that extends infinitely through space.

For the first point, the situation is a little trickier. Speaking purely formally, the wavefunction can exist outside of the light cone, so even if you introduce a finite speed of light built-in to the theory, your particle will be able to break this spead limit with exponential probability. However this is purely an illusion... if you work in the Heisenberg picture, you find that all particle operators commute or anticommute at spacelike separations, and you prevent your theory from violating local causality.
 
Thanks for the reply, the only thing that doesn't make sense is that you say "it is impossible to get a single wavefunction that extends infinitely through space" since it would take an infinite potential to stop a wavefunction completely.
I first thought about all this when CERN announced the superluminal neutrinos. But if I understand correctly, "time tunneling" of particles is excluded already because of the nature of the operators.
 
ihatelolcats said:
Thanks for the reply, the only thing that doesn't make sense is that you say "it is impossible to get a single wavefunction that extends infinitely through space" since it would take an infinite potential to stop a wavefunction completely.

No probs! It's an interesting question. Your point is incorrect, suppose I have a particle with momentum p moving through empty space (there is no local potential). We cannot have a pure state with momentum p since the particle has not existed for infinite time, rather, its a superposition of waves with momenta concentrated within a band of width \Delta p. Such a wave propagates through space with some finite velocity which is group velocity of the wave (v = dE/dp), but it is localized within a region of space of size \Delta x = \frac{\hbar}{\Delta p} (This is the Heisenberg uncertainty relation). The wave absolutely does not extend infinitely through space.. and this is totally consistent with our usual observation of electrons in metals for example.. electrons are delocalized, but even when you get to the superconducting regime, the wavefunction of an electron does not extend beyond some typical length which is much much smaller than the size of the sample.
 

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