Bell made Simple - Hardy result

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In summary, a new B thread has been created for people to discuss and learn from. This thread aims to clarify confusing issues that have arisen in the "CFD - Counterfactual Definiteness" thread. The example discussed is from Hardy, where a joint-entanglement-measurement at spacelike separation with two settings (1 and 2) and outcomes (YES or NO) has been shown to have certain configurations that result in forbidden outcomes. This is similar to the CHSH inequality, but more complicated. A circuit has been proposed that meets the desired criteria, with a partially-entangled state and controlled-Hadamard gates. The resulting grid of outputs has holes in certain cells, but the cell for (A1
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Eye_in_the_Sky
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I am starting this B thread for people to discuss and learn from.

In particular, I am hoping it will help to clarify some of the confusing issues which have come up in the "CFD - Counterfactual Definiteness" thread.

"Well wishings to ALL, for a complete and successful understanding!"
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The example below is due to Hardy.
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Each of the instruments of Alice and Bob (which together perform a joint-entanglement-measurement at spacelike separation) have two settings, 1 and 2, for which the outcomes can be YES or NO.

There is a quantum-mechanical entanglement scenario for which each of the following statements is true:

(0) For the configuration <a1,b1>: the outcome (NO,NO) is sometimes obtained.

(1) For the configuration <a1,b2>: if a1 gives NO, then b2 gives YES with certainty.

(2) For the configuration <a2,b1>: if b1 gives NO, then a2 gives YES with certainty.

(3) For the configuration <a2,b2>: the outcome (YES,YES) is forbidden.
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I have taken this example (but adapted the notation) from Penrose's "Road to Reality", §23.5, p. 590. There, he mentions that the (NO,NO) outcome for the setting in (0) is obtained with a probability of 1/12.
 
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Here's a circuit that meets the desired criteria:

Screenshot from 2016-09-09 12:42:34.png


The first gate is just making a 1/3-2/3 split. Its matrix is {{√⅔,-√⅓},{√⅓,√⅔}}. Then the controlled-Hadamard finishes the setup of the shared partially-entangled state ##|00\rangle + |01\rangle + |10\rangle##. Later, the referees make their choice of which case to query via a Hadamard+measure. Then the players can apply operations that depend on the choice of their referee; they both do nothing in the ON case and apply H+X in the OFF case.

Note the grid of outputs to the right. Imagine splitting it up into four 2x2 blocks. The top-left block is the A1,B1 case. Top-right is A1,B2. Bottom-left is A2,B1. Bottom-right is A2,B2. Within each 2x2 block the top-left is NO,NO and the bottom-right is YES,YES.

There's holes over the cells corresponding to (A2,B1,NO,NO), (A1,B2,NO,NO), and (A2,B2,YES,YES). But the cell for (A1,B1,NO,NO) isn't empty. Those are the requirements.
 

FAQ: Bell made Simple - Hardy result

What is the Bell made Simple - Hardy result?

The Bell made Simple - Hardy result is a mathematical theorem that proves the impossibility of a local hidden variable theory in explaining the outcomes of quantum entanglement experiments.

Who discovered the Bell made Simple - Hardy result?

The Bell made Simple - Hardy result was discovered by British physicist John Stewart Bell in 1964.

What is quantum entanglement?

Quantum entanglement is a phenomenon in quantum mechanics where two or more particles become connected in such a way that the state of one particle affects the state of the other, even when they are separated by a large distance.

Why is the Bell made Simple - Hardy result significant?

The Bell made Simple - Hardy result is significant because it provides strong evidence against the existence of local hidden variables, which were once considered a possible explanation for the seemingly bizarre behavior of quantum entangled particles.

How does the Bell made Simple - Hardy result impact our understanding of quantum mechanics?

The Bell made Simple - Hardy result challenges the traditional understanding of quantum mechanics and suggests that there may be other underlying principles at play in the quantum world that we have yet to fully comprehend.

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