Thermal interpretation and Bell's inequality

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Discussion Overview

The discussion revolves around the thermal interpretation (TI) of quantum mechanics and its ability to explain a specific transition in Bell's 1964 paper regarding the derivation of Bell's inequality. Participants are examining the implications of Bell's equations and the assumptions involved in moving from one equation to another, particularly in the context of quantum mechanics.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question how the thermal interpretation can explain Bell's transition from the first to the second equation, suggesting that it involves assumptions that quantum mechanics (QM) violates.
  • Others argue that the transition is a standard expectation value calculation and does not require TI for explanation.
  • A participant points out that Bell explicitly states the assumption in his paper, which is critical for understanding the transition.
  • There is a discussion about the physical significance of Bell's use of his first equation, with some seeking deeper insights into its implications.
  • Some participants assert that Bell's reasoning is clear and does not depend on any interpretation of QM, while others express confusion about the specifics of how Bell uses his equations.
  • One participant emphasizes the need to understand the physical significance of Bell's approach to using his first equation in the context of the derivation.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the thermal interpretation can adequately explain Bell's transition between equations. There are competing views regarding the relevance of TI and the clarity of Bell's reasoning.

Contextual Notes

Participants reference specific equations and assumptions from Bell's paper, indicating that the discussion is deeply rooted in the technical details of the derivation of Bell's inequality. The conversation reflects varying levels of understanding and interpretation of the material.

  • #61
For PeterDonis: Of course! Many thanks and my apologies! The problem occurs lower down! Let me redefine it using {.} to keep related terms together:

From the first eqn in Post #51 above, including the integrals in line with Bell (1964):​
$$E(a,b)-E(a,c)=-\smallint d\lambda \rho(\lambda)\left[\{A(a, \lambda)A(b, \lambda)\}-\{A(a, \lambda)A(c, \lambda)\}\right]\;\;(1)$$
$$=-\smallint d\lambda \rho(\lambda)\{A(a, \lambda)A(b, \lambda)\}\left[1-\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(c, \lambda)\}\right].\;\;(2)$$
$$So, since \;A(a, \lambda)A(b, \lambda)\leq1: \;\;(3)$$
$$ |E(a,b)-E(a,c)|\leq\smallint d\lambda \rho(\lambda)\left[1-\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(c, \lambda)\}\right]\;\;(4)$$
$$\leq1-E(a,b)E(a,c).\;\;(5)$$

Now, in eqn (4), if I used ##A(a, \lambda)A(a, \lambda)=1##, I would get Bell's inequality; just like you and DarMM and many others do using ##A(b, \lambda)A(b, \lambda)=1## in the alternative formulation in Post #51.

But then I would have converted (5) -- by an improper separation of terms* -- from an inequality that is never false into Bell's inequality which is frequently false.

* By an improper separation I mean this: I would have converted ##E(a,b)E(a,c)## into ##E(b,c)##; which is unlikely to be true. That a function ##F(b,c)## should equal a function ##F(a,b)F(a,c)## over all ##a,b,c##.

The above should show why I am still seeking to understand the mathematics behind Bell's theorem.

My question: Given the above, does Bell's inequality ##
|E(a,b)-E(a,c)|\leq1+E(b,c)
## arise from an improper mathematical separation of terms?
 
Last edited:
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  • #62
N88 said:
From the first eqn in Post #51 above, including the integrals in line with Bell (1964):
$$E(a,b)-E(a,c)=-\smallint d\lambda \rho(\lambda)\left[\{A(a, \lambda)A(b, \lambda)\}-\{A(a, \lambda)A(c, \lambda)\}\right]\;\;(1)$$
$$=-\smallint d\lambda \rho(\lambda)\{A(a, \lambda)A(b, \lambda)\}\left[1-\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(c, \lambda)\}\right].\;\;(2)$$
$$So, since \;A(a, \lambda)A(b, \lambda)\leq1: \;\;(3)$$
$$ |E(a,b)-E(a,c)|\leq\smallint d\lambda \rho(\lambda)\left[1-\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(c, \lambda)\}\right]\;\;(4)$$
$$\leq1-E(a,b)E(a,c).\;\;(5)$$

Now, in eqn (4), if I used ##A(a, \lambda)A(a, \lambda)=1##, I would get Bell's inequality; just like you and DarMM and many others do using ##A(b, \lambda)A(b, \lambda)=1## in the alternative formulation in Post #51.

But then I would have converted (5) -- by an improper separation of terms* -- from an inequality that is never false into Bell's inequality which is frequently false.

* By an improper separation I mean this: I would have converted ##E(a,b)E(a,c)## into ##E(b,c)##; which is unlikely to be true. That a function ##F(b,c)## should equal a function ##F(a,b)F(a,c)## over all ##a,b,c##.
I'm genuinely having a hard time understanding this. Where have you shown that ##E(a,b)E(a,c)## can be converted into ##E(b,c)##? I'm not following.

Also how do you get from your equation (1) to your equation (2)? Your equations are not mine or those given by Bell. Where are you getting them from?
 
  • #63
DarMM said:
I'm genuinely having a hard time understanding this. Where have you shown that ##E(a,b)E(a,c)## can be converted into ##E(b,c)##? I'm not following.

In (4), if we let ##\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(c, \lambda)\}## reduce to ##A(b, \lambda)A(c, \lambda)## by allowing ##A(a, \lambda)A(a, \lambda)=1,## (as stated) then the integral gives ##-E(b,c) ##. It is similar to the way you get the same final result.

You and I and Bell start and finish at the same point IF we allow that reduction. Noting that such a reduction moves us from a totally valid inequality to Bell's partially valid inequality.

DarMM said:
Also how do you get from your equation (1) to your equation (2)? Your equations are not mine or those given by Bell. Where are you getting them from?

Eqn (1) = eqn (2) by algebra, by way of ##\{A(a, \lambda)A(b, \lambda)\}\{A(a, \lambda)A(b, \lambda)\} = 1.##

Peter stressed that Bell's inequality is mathematical. So I am trying to understand how the mathematics goes from a physically valid start to a result that is false under QM.
 
  • #64
N88 said:
I am trying to understand how the mathematics goes from a physically valid start

You continue to miss the point: since the whole derivation is just a mathematical proof, if the conclusion doesn't match QM, the starting point doesn't either. In other words, what Bell is showing is that his starting point is not physically valid. It looks like it ought to be physically valid, but it isn't.

Since you appear unable to grasp this simple point despite numerous attempts to explain it, there is no point in continuing this thread. Thread closed.
 
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