By Lewis B.

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E clearest memory I have concerning quantum theory from college did not come from a physics course, but rather from reading Bernard d’Espagnat’s account of Bell’s theorem and Aspect’s experiments in the Scienti c American. Bell’s argument was crisp and clear, and the experimental results appeared decisive. My roommates at the time still recall seeing me pacing the room, article in hand, going around and around in circles. e violations of Bell’s inequality were my lodestar, a sharp-edged result that could guide us to a deeper understanding of space and time.

To be sure, it was an endurance contest: I really didn’t like physics the way most physics students do, and I suppose more than one hiring committee noticed that. So, blame it on Heinz Pagels’s prose, John Wheeler’s inspiration, and the San Antonio, Texas, television stations. Quantum theory has taken my heart since the beginning because of its spicy mélange of law . . without law. In a world where the laws of nature are as mutable as the laws of legislatures, most anything might happen. Imagine that!

Is was my strong impression. Shimony referred to this sort of thing as a “peaceful coexistence” between relativity and quantum theory. To me, it seemed like a dark and uneasy conspiracy that cried out for an explanation. I started to form the vague idea that the hidden-variable level must be in a state of some sort of statistical equilibrium, in which the nonlocal effects average to zero. In ordinary statistical mechanics, thermal equilibrium yields nely tuned relations such as detailed balancing, the uctuation–dissipation theorem, and so on.

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The Uni-Molecular Decomposition of Azo-Methane; the Adequacy of Activation by Collision by Lewis B.


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