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In the Beginning was Information

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uncertainties is always greater than a specific natural constant,which would have been impossible if <strong>the</strong> uncertainties were vanishinglysmall. It follows for example that certain measurementscan never be absolutely exact. This finding resulted in <strong>the</strong> collapseof <strong>the</strong> structure of <strong>the</strong> <strong>the</strong>n current nineteenth century deterministicphilosophy. The affirmations of <strong>the</strong> laws of nature are so powerfulthat viewpoints which were held up to <strong>the</strong> time <strong>the</strong>y are formulated,may be rapidly discarded.<strong>In</strong>formation <strong>the</strong>orems: <strong>In</strong> conclusion we mention that <strong>the</strong>re is aseries of <strong>the</strong>orems which should also be regarded as laws of nature,although <strong>the</strong>y are not of a physical or a chemical nature. Theselaws will be discussed fully in this book, and all <strong>the</strong> previouslymentioned criteria N1 to N9 as well as <strong>the</strong> relevance statements R1to R6, are also valid in <strong>the</strong>ir case.2.6 Possible and Impossible EventsThe totality of all imaginable events and processes can be dividedinto two groups as in Figure 7, namelya) possible eventsb) impossible events.Possible events occur under <strong>the</strong> “supervision” of <strong>the</strong> laws ofnature, but it is in general not possible to describe all of <strong>the</strong>m completely.On <strong>the</strong> o<strong>the</strong>r hand, impossible events could be identified bymeans of <strong>the</strong> so-called impossibility <strong>the</strong>orems.Impossible events can be divided into two groups, those which are“fundamentally impossible”, and those which are “statisticallyimpossible”. Events which contradict for example <strong>the</strong> energy law,are impossible in principle, because this <strong>the</strong>orem even holds forindividual atoms. On <strong>the</strong> o<strong>the</strong>r hand, radio-active decay is a statisticallaw which is subject to <strong>the</strong> probability <strong>the</strong>orems, and cannotbe applied to individual atoms. But in all practical cases <strong>the</strong> numberof atoms is so immense that an “exact” formulation can beused, namely n(t) = n 0 x e -k x t . The decay constant k does notdepend on temperature, nor on pressure, nor on any possible chem-40

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