Abstract
AbstractIn 1927, Paul Dirac first explicitly introduced the idea that electrodynamical processes can be evaluated by decomposing them into virtual (modern terminology), energy non-conserving subprocesses. This mode of reasoning structured a lot of the perturbative evaluations of quantum electrodynamics during the 1930s. Although the physical picture connected to Feynman diagrams is no longer based on energy non-conserving transitions but on off-shell particles, emission and absorption subprocesses still remain their fundamental constituents. This article will access the introduction and the initial reception of this picture of subsequent transitions (PST) by conceiving of concepts, models, and their representations as tools for the practitioners. I will argue for a multi-factorial explanation of Dirac’s initial, verbally explicit introduction: the mathematical representation he had developed was highly suggestive and already partly conceptualized; Dirac was philosophical flexible enough to talk about transitions when no actual transitions, according to the general interpretation of quantum mechanics of the time, occurred; and, importantly, Dirac eventually used the verbal exposition in the same paper in which he introduced it. The direct impact of PST on the conception of quantum electrodynamical processes will be exemplified by its reflection in diagrammatical representations. The study of the diverging ontological commitments towards PST immediately after its introduction opens up the prehistory of a philosophical debate that stretches out into the present: the dispute about the representational and ontological status of the physical picture connected to the evaluation of the perturbative series of QED and QFT.
Funder
Deutsche Forschungsgemeinschaft
Publisher
Springer Science and Business Media LLC
Subject
History and Philosophy of Science,Mathematics (miscellaneous)
Reference102 articles.
1. Akhiezer, A., and I. Pomeranchuck. 1937. Kohaerente Streuung von Gamma-Strahlen durch Kerne. Physikalische Zeitschrift der Sowjetunion 11: 478–498.
2. Amaldi, E. 1929. Sulla teoria quantistica dell’effetto Raman. Rendiconti Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali 9: 876–881.
3. Amaldi, E., and E. Segré. 1929. Sulla teoria dell’effetto Raman. Rendiconti Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali 9: 407–409.
4. Bhabha, H. 1940. On elementary heavy particles with any integral charge. Proceedings of the Indian Academy of Science 11: 347–368. https://doi.org/10.1007/BF03051350.
5. Blum, A. 2017. The state is not abolished, it withers away: How quantum field theory became a theory of scattering. Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 60: 46–80. https://doi.org/10.1016/j.shpsb.2017.01.004.
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