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Studies in History and Philosophy of Science Part B Studies in History and Philosophy of Modern Physics

On classical cloning and no-cloning

Nicholas J. Teh

Published Feb 1, 2012• 4 citations
Publisher
DOI
10.1016/j.shpsb.2011.11.005

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The quantum no cloning theorem is an essential result in quantum information theory. Following this idea, we give a physically natural definition of cloning in the context of classical mechanics using symplectic geometry, building on work of A. Fenyes, J. Math. Phys. 53, 012902 (2012). We observe, following Fenyes, any system with phase space (R2N,dxi∧dyi) can be cloned in our definition. However, we show that if (M, ω) can be cloned in our definition, then M must be contractible. For instance, this shows the simple pendulum cannot be cloned in Hamiltonian mechanics. We further formulate a robust notion of approximate cloning, and show that if (M, ω) can be approximately cloned, then M is contractible. We give interpretations of our results and in some special cases reconcile our no cloning theorems with the general experience that classical information is clonable. Finally we point to new directions of research, including a connection of our result with the classical measurement problem.