Cluster decomposition and EPR correlations

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Discussion Overview

The discussion centers on the compatibility of Weinberg's 'cluster decomposition' principle with EPR correlations observed in entangled states. Participants explore theoretical implications, interpretations, and potential reformulations of the principle in the context of quantum field theory (QFT) and quantum mechanics (QM).

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants express concern that Weinberg's formulation of the cluster decomposition principle is incompatible with EPR correlations, suggesting that the principle may need reformulation to align with these correlations.
  • Others argue that the cluster decomposition principle, as interpreted in QFT, can be valid if certain conditions regarding the factorization of states are met, particularly in the context of spatially separated subsystems.
  • A participant highlights that the principle's application requires all relevant quantities to be measured in both the initial and final states, which complicates its use in EPR-type experiments.
  • Some participants reference Weinberg's own statements regarding the principle, noting that they seem to contradict the existence of EPR correlations.
  • There is mention of decoherence as a potential factor that could reconcile the cluster decomposition principle with EPR correlations, though details on this connection are not fully explored.
  • Links to external resources, including Weinberg's book and relevant papers, are shared for further exploration of the topic.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the compatibility of the cluster decomposition principle with EPR correlations. Multiple competing views are presented, with some defending the principle's validity under certain conditions, while others challenge its formulation as stated by Weinberg.

Contextual Notes

Limitations in the discussion include assumptions about the separability of states and the necessity of measuring all relevant indices, which are not fully resolved. The implications of decoherence in this context remain speculative.

metroplex021
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Does anyone know of a good discussion of the compatibility (or otherwise) of Weinberg's 'cluster decomposition' principle with the fact that entangled states yield distant but correlated measurements?
 
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Salman2 said:
Here is a link to the topic from Weinberg's 1995 book--found on internet:

http://books.google.com/books?id=3w...page&q=weinberg cluster decomposition&f=false

Thanks for this - a useful link for future reference. But for now I'm looking specifically for discussion of CD and its relation to EPR-type correlations of distant measurement results, and to my knowledge, Weinberg doesn't discuss that here (which seems a strange oversight to me).
 
The cluster decomposition principle is an interpretation of the factorization of the S matric for separated reaction :
if S_{\alpha_1,\beta_1} corresponds to the amplitude for \alpha_1\rightarrow\beta_1
and S_{\alpha_2,\beta_2} corresponds to the amplitude for \alpha_2\rightarrow\beta_2
then S_{\alpha_1\alpha_2,\beta_1\beta_2}=S_{\alpha_1,\beta_1}S_{\alpha_2,\beta_2}
Each label indicates a specification for all particles in the initial (final) state, including momenta, spins, particle species, and anything else relevant to fully specify a particle state.

Now in an EPR-type experiment, we do not have independent reactions. We have only one final state which is not separable. Since we already cannot separate the state in QM, we have no reason to attempt to separate it in QFT and hope to get a sensible result. The problem is not with the cluster decomposition principle. The problem is with the thought experiment itself. It is generally necessary to assume that all relevant quantities are measured both in the prepared initial and the detected final state.
 
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I think that the cluster decomposition principle (CDP) IN THE FORM EXPRESSED BY WEINBERG is wrong.

Indeed, in Sec. 4.3 Weinberg explicitly says:
"It is one of the fundamental principles of physics ... that experiments that are sufficiently separated in space have unrelated results."
...
"... the cluster decomposition principle states that if multi-particle processes ... are studied in N very distant laboratories, then the S-matrix element for the overall process factorizes."

Clearly, these statements formulated as such are incompatible with EPR correlations, and are therefore wrong.

Yet, it does not mean that CDP cannot be reformulated in a more careful way, such that it becomes compatible with EPR correlations. After all, a form of the CDP principle can be derived from QFT, and QFT is compatible with EPR correlations. Probably, CDP can be viewed as a consequence of QFT & decoherence, but I am not aware of any detailed discussion of that idea.
 
humanino said:
The cluster decomposition principle is an interpretation of the factorization of the S matric for separated reaction :
if S_{\alpha_1,\beta_1} corresponds to the amplitude for \alpha_1\rightarrow\beta_1
and S_{\alpha_2,\beta_2} corresponds to the amplitude for \alpha_2\rightarrow\beta_2
then S_{\alpha_1\alpha_2,\beta_1\beta_2}=S_{\alpha_1,\beta_1}S_{\alpha_2,\beta_2}
Each label indicates a specification for all particles in the initial (final) state, including momenta, spins, particle species, and anything else relevant to fully specify a particle state.

Now in an EPR-type experiment, we do not have independent reactions. We have only one final state which is not separable. Since we already cannot separate the state in QM, we have no reason to attempt to separate it in QFT and hope to get a sensible result. The problem is not with the cluster decomposition principle. The problem is with the thought experiment itself. It is generally necessary to assume that all relevant quantities are measured both in the prepared initial and the detected final state.
I would summarize and formalize it this way:
CDP says that if
1. the initial state (of spatially separated subsystems) can be factorized
and
2. the subsystems remain spatially separated all the time
then
the final state can also be factorized.

This is a correct form of CDP in QFT. But this is not the form explicitly stated by Weinberg.
 
Demystifier said:
This is a correct form of CDP in QFT. But this is not the form explicitly stated by Weinberg.
There are quite some caveats with scattering theory alone, and one must assume that all relevant indices are measured or otherwise summed over. That is assumed when we say that we prepare an initial state. It is not sufficient to use half of the final state of an EPR-type experiment, which would be inseparable from another half somewhere else. In this situation, once the initial state (half final state of an EPR exp.) has been measured it becomes separated and the CDP applies.
 
Yes, that is essentially what I had in mind when I mentioned decoherence in post #5.
 
  • #10
Thanks everyone for those replies. I'm glad it's not just me who thinks it's a bit odd. I'm going to keep looking for somewhere that Weinberg himself addresses (what seems to me) his strange wording of this principle. But any other refs would be really appreciated of course.
 

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