Abstract
Variational principles for dynamical systems have a long history. Although precursors go back at least to Leibnitz (see for example (Euler 1752)) and Euler (1744) the “principle of least action” was given modern form by de Maupertuis (1744, 1746). We will not attempt to trace the history here; a brief useful account is given in Sommerfeld’s lectures (Sommerfeld 1964). The most important names in the history of the development of dynamical systems, or at least those that will bear most directly on the following discussion, are those of Lagrange (1788) and Hamilton (1834, 1835).
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For complex reasons, Schwinger’s influence on modern physics is not widely appreciated. His contributions to our current understanding of nature are underrepresented in textbooks, with some notable exceptions (Toms 2007).
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Milton, K.A. (2015). Historical Introduction. In: Schwinger's Quantum Action Principle. SpringerBriefs in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-20128-3_1
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DOI: https://doi.org/10.1007/978-3-319-20128-3_1
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