Entanglement, classical correlation, and questions about superluminal signalling

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Discussion Overview

The discussion revolves around the relationship between entanglement, classical correlation, and the implications for superluminal signaling. Participants explore whether questions about superluminal signaling are fundamentally tied to entanglement or if they also apply to classical correlations. The scope includes theoretical considerations and conceptual clarifications regarding quantum mechanics and classical physics.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions if the typical questions about superluminal signaling are fundamentally about entanglement or if they could apply to any form of correlation, including classical correlation.
  • Another participant suggests that if there is no entanglement and the state is separable, it seems 'obvious' that superluminal signaling cannot occur.
  • A different perspective reformulates the question by considering a scenario where Alice sends a random signal to Bob, questioning whether this could be used to send a useful signal, concluding that random signals are not useful.
  • Some participants express uncertainty about the implications of correlations in separable states, suggesting that the questions posed may not delve deeper than the correlation itself.
  • There is a discussion about the nature of the state of Bob's spin before Alice's measurement and the implications of superluminal signaling in this context.

Areas of Agreement / Disagreement

Participants do not reach a consensus. There are competing views on whether the questions about superluminal signaling are adequately addressed by classical correlation or if they are uniquely tied to entanglement. Some participants agree on the separability condition but differ in their interpretations of its implications.

Contextual Notes

Limitations include the dependence on definitions of entanglement and classical correlation, as well as unresolved questions about the nature of correlations in separable states. The discussion also highlights the ambiguity in the usefulness of random signals in the context of superluminal communication.

Physics Monkey
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The quantum physics forum is full of questions about why entanglement can't be used to signal superluminally.

My question is this: do these questions usually still make sense if we replace entanglement by classical correlation? For example, I can send Alice and Bob each a random bit but with both bits perfectly correlated. At the level of the typical entanglement/superluminal signaling question, are these any different e.g. since Alice has the same (completely mixed) state in both case? I realize this is a bit soft, so your opinions and impressions are very welcome. Basically what I want to know is if people are really asking about entanglement or merely any kind of correlation.

And let me clear, I am certainly very aware that entanglement is not the same as classical correlation, and of Bell's theorem, and so on. In my mind, this question is really about the very basic issues and about pedagogy.
 
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I probably didn't understand your question, but if there is no entanglement i.e. if the state is separable, then isn't 'obvious' that there cannot be superluminal signaling?
 
I would reformulate the Physics Monkey's question in the following way. Assume that Alice is correlated with Bob through a superluminal signal sent from Alice to Bob. Assume further that this signal is chosen randomly, i.e., not freely chosen by Alice. The questions is: Can Alice use it to send a USEFUL signal to Bob? The answer is no, because random signals are not useful.
 
martinbn said:
I probably didn't understand your question, but if there is no entanglement i.e. if the state is separable, then isn't 'obvious' that there cannot be superluminal signaling?

Perhaps so, and this is sort of what I was trying to get at. Most of the questions I've seen seem to be using nothing more than the fact that outcomes are correlated (plus the spooky language of particles deciding what to do based on their distant counterpart's measured state) as some of kind of suggestion of superluminal signaling.

The state I described is separable but still correlated: \rho = \frac{1}{2} |\uparrow \rangle \langle \uparrow |_A |\uparrow \rangle \langle \uparrow |_B + \frac{1}{2}|\downarrow \rangle \langle \downarrow |_A |\downarrow \rangle \langle \downarrow |_B. My feeling is that these sorts of questions aren't using anything more than the correlation displayed here.

What I'm trying to do is understand whence these questions about entanglement originate. Is it a bad metaphor we're using?
 
Demystifier said:
I would reformulate the Physics Monkey's question in the following way. Assume that Alice is correlated with Bob through a superluminal signal sent from Alice to Bob. Assume further that this signal is chosen randomly, i.e., not freely chosen by Alice. The questions is: Can Alice use it to send a USEFUL signal to Bob? The answer is no, because random signals are not useful.


This is an interesting reformulation. At the level of comparing correlated outcomes, one could imagine that Alice measuring the state of her spin really does set the state of Bob's spin via superluminal signal. But its not clear to me what the state of Bob's (classical?) spin is before Alice's measurement. It is probably also important that this superluminal state resetting can only happen once and that Bob can't actually determine when it happened.
 

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