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Titlebook: An Axiomatic Basis for Quantum Mechanics; Volume 1 Derivation Günther Ludwig Book 1985 Springer-Verlag Berlin Heidelberg 1985 Mechanics.Sp

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https://doi.org/10.1007/978-3-658-42642-2eories. Therefore, we cannot start with a set . interpreted as a set of microsystems as in [2] (see [3] § 5 for abbreviated formulations such as “set of microsystems”). We rather “question” the existence of a microsystem, i.e. we will theoretically retrace the discovery of microsystems. In the theor
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Die Methode der finiten Elementehen we have forgotten “too much” to describe physical systems as effect carriers. Let us try to amend this by introducing the concepts “observable” and “preparator”. These concepts represent abstract and idealized residues from the structure of preparation and registration procedures. Without fallin
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https://doi.org/10.1007/978-3-642-57250-0 characterize the directed actions in nature. Hence, we must add axioms (laws in the sense of [3] § 7.3) and thus try to approach (by standard extension in the sense of [3] § 8) a g. G.-closed theory of “microsystems”. Here, the word “microsystem” is to characterize (initially inexactly) the fundame
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978-3-642-70031-6Springer-Verlag Berlin Heidelberg 1985
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Erratum to: Der Tauschwerth des Waldbodens,In [3], [30] and [48] we formulated the objective of finding, for a physical theory, an axiomatic basis with “physically interpretable axioms” (see [30] and XIII § 2), wherein the physical laws appear distinctly and whereby the problems of interpretation can be solved clearly. In this book, we attack this objective for quantum mechanics.
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https://doi.org/10.1007/978-3-658-42642-2Since we intend to develop an axiomatic basis for quantum mechanics, we must delve into the pretheories for quantum mechanics in order to describe the fundamental domain of quantum mechanics (see [1] III §§ 2 and 4; or, to be precise, [3] §§ 3 and 5). Nevertheless, to understand the following it is not necessary to have read [1] or [3] or [30].
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