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In 1901, the German physicist Max Planck (1858–1947) proposed a solution. It is superseded by relativistic mechanics for systems moving at large velocities near the speed of light, quantum mechanics for systems at small distance scales, and relativistic quantum field theory for systems with both properties. I don’t believe this is even coherent (in a Feynman approach). Suppose, for example, that we start S* in its ground state, and S in the state and it follows from the fact that S* is a measuring instrument for A, and the linearity of U that their combined state after interaction, is This, however, is inconsistent with the dynamical rule for contexts of type 2, for the dynamical rule for contexts of type 2 (and if there are any such contexts, this is one) entails that the state of the pair after interaction is either Indeed, it entails that there is a precise probability of 1/2 that it will end up in the former, and a probability of 1/2 that it will end up in the latter.

Pages: 414

Publisher: Echo Point Books & Media; Reprint ed. edition (November 10, 2015)

ISBN: 1626543011

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