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The experiment of Greenberger, Horne, and Zeilinger Print
The bare facts

Please read this first.

Yet there is a failsafe strategy without pre-agreed answers.

Here goes:

  • Andy, Bob, and Charles prepare three particles (say, electrons) in a particular quantum state, which defining joint probability distributions over possible measurement outcomes. The probabilities are independent of the distances between the particles.
  • Each player takes one of these particles.
  • Whoever is asked the X question measures the x component of the spin of his particle (which has two possible values, which we will take to be +1 and –1) and answers with his outcome. Whoever is asked the Y question measures the y component of the spin of his particle and answers likewise.
  • Proceeding in this manner, Andy, Bob, and Charles are sure to win every time.

Time for our next million dollar question! Is it possible for the x and y components of the spins of the three particles to be in possession of values even if no values are actually measured?

 

RFA image 

Caustic Sea (detail) by Eric J. Heller.

 

Right, the answer is again negative. For the same reason that there can be no strategy with pre-agreed answers, there can be no pre-existent values.

To check this, let us assume — contrary to the facts — that spin components have values irrespective of what is and what is not measured. And suppose that the y components of the three spins have been measured, and that the following values were obtained: YA, YB, YC. (These expressions now stand for specific values, either +1 or –1.)

Since the product XA YB YC is sure to come out equal to 1, we are entitled to conclude that if we had measured XA instead of YA, we would have obtained XA= (YB YC)–1.

By the same token we are entitled to conclude that if we had measured XB instead of YB, we would have obtained XB= (YA YC)–1, and that if we had measured XC instead of YC, we would have obtained XC= (YA YB)–1.

Ergo, if we had measured all three x components instead of the three y components, the product of the outcomes would have been

(YB YC)–1 (YA YC)–1 (YA YB)–1 = +1.

Remember, (YA)2 = (YB)2 = (YC)2 = 1.

Once again the assumption that observables — measurable physical quantities — have values whether or not they are measured, has led us down the garden path, for each time we measure the three x components, their product is invariably –1.

 

RFA image

Caustic Sea (detail) by Eric J. Heller.

 

Based on D.M. Greenberger, M.A. Horne, and A. Zeilinger, "Going beyond Bell's theorem," in Bell's Theorem, Quantum Theory, and Conceptions of the Universe, edited by M. Kafatos (Dordrecht: Kluwer, 1989), pp. 69–72.

 

 
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