Abstract
The principle of superposition has long plagued the quantum mechanics of macrosopic bodies. Macroscopic objects are taken to be composed of a large number of interacting constituents, each in its interaction with others governed by the laws of quantum mechanics. For any two systems already represented, quantum theory represents the composite by a vector in the tensor product of the Hilbert spaces representing the systems separately. Thus, an n-body system is represented by a vector in the Hilbert space \( {H^n} = {H_I} \otimes {H_{II}} \otimes ... \otimes {H_N} \). When n becomes large enough to constitute a macroscopic body the treatment is problematic. Macroscopic states, it appears, do not superpose. Macroscopic bodies seem to possess sharp values for all observable quantities simultaneously.
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© 1976 Springer Science+Business Media Dordrecht
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Cartwright, N.D. (1976). Superposition and Macroscopic Observation. In: Suppes, P. (eds) Logic and Probability in Quantum Mechanics. Synthese Library, vol 78. Springer, Dordrecht. https://doi.org/10.1007/978-94-010-9466-5_11
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DOI: https://doi.org/10.1007/978-94-010-9466-5_11
Publisher Name: Springer, Dordrecht
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