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N. David Mermin
David Mermin is professor emeritus of physics at Cornell University. He is perhaps best known for his contributions to the foundations of physics, especially his mechanisms for describing Bell's Theorem, his contributions to quantum information science, and his defense of QBism.
In !985, Mermin wrote the very popular and widely cited paper "Is the Moon There When Nobody Looks?" in In the paper Mermin described what he called a "very simple version" of John Bell's gedanken experiment. Mermin says his "EPR Apparatus" exhibits all the experimental behavior of Bell's version, without any reference to the "underlying mechanism that makes the gadget work." He provides samples of (hypothetical) data produced by the apparatus, which presumably matches (statistically) the data produced in real experimental tests of Bell's Theorem.
A few years later, Mermin published a variation on his original apparatus at a 1987 Notre Dame conference on Bell's Theorem. In this work, "More Experimental Physics from EPR," his new device has different switch settings but more data is provided to exhibit the mysterious entanglement (perfect correlations) between widely separated measurements. In this paper, Mermin gave a definite answer to his earlier question about the moon, "We now know that the moon is demonstrably not there when nobody looks." (p.50)
Perfect Correlations Depend on Polarizer Angles
Can Perfect Correlations Be Explained by Conservation Laws?
David Bohm, Eugene Wigner, and even John Bell suggested that conservation of angular momentum (or particle spin) tells us that if one spin-1/2 electron is measured up, the other must be down. Albert Einstein used conservation of linear momentum in his development of the EPR Paradox.
David Bohm wrote in 1957, We consider a molecule of total spin zero consisting of two atoms, each of spin one-half. The wave function of the system is therefore Eugene Wigner wrote in 1962 If a measurement of the momentum of one of the particles is carried out — the possibility of this is never questioned — and gives the result John Bell wrote in 1964, With the example advocated by Bohm and Aharonov, the EPR argument is the following. Consider a pair of spin one-half particles formed somehow in the singlet spin state and moving freely in opposite directions. Measurements can be made, say by Stern-Gerlach magnets, on selected components of the spins
Just like Bohm and Wigner, Bell is
Albert Einstein made the same argument in 1933, shortly before EPR, though with conservation of Suppose two particles are set in motion towards each other with the same, very large, momentum, and they interact with each other for a very short time when they pass at known positions. Consider now an observer who gets hold of one of the particles, far away from the region of interaction, and measures its momentum: then, from the conditions of the experiment, he will obviously be able to deduce the momentum of the other particle. If, however, he chooses to measure the position of the first particle, he will be able tell where the other particle is.
Supporters of the Copenhagen Interpretation (including Mermin?) claim that the properties of the particles (like angular or linear momentum) In our case, the entangled particles have been prepared in a superposition of states, both of which have total spin zero.
ψ = (1/√2) [ ψ ]
_{+} (1) ψ_{-} (2) - ψ_{-} (1) ψ_{+} (2)
So whichever of these two states is
Wolfgang Pauli called it a "measurement of the first kind" when a system is As long as nothing interferes with either entangled particle as they travel to the distant detectors, they will be found to be perfectly correlated if (and only if) they are measured at the same angle. Otherwise. the correlations should fall off as the square of the cosine of the angle difference. Oddly, Bell's inequality predicts a linear falloff with the angle difference, and a strange non-physical "kink" at angles 0°, 90°, 180°, and 270° (which Bell himself pointed out).
References
"Is the Moon There When Nobody Looks? Reality and the Quantum Theory." Physics Today 38.4 (1985): 38-47.
"More Experimental Physics from EPR," in
"What is Quantum Mechanics Trying to Tell Us?,"
"An Introduction to QBism," |