Abstract
In this chapter I will show how Feynman used diagrams to represent and modify physical models of electrons (and later their interaction) and how he used these representations to derive quantitative expressions that are “true of the model”.
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Notes
- 1.
Cartwright (1983).
- 2.
- 3.
Dirac (1935, p. 260).
- 4.
- 5.
See, e. g., Galison (1998).
- 6.
Dirac Equation a, folio 27.
- 7.
Dirac Equation a (1946/47a, folio 1), (Feynman’s page numbering: 1), see Fig. 4.10; cf. Schweber (1994a, p. 406). Feynman’s letter was written on a “Monday February 10”. Around the time in question, February 10 was a Monday in 1941, 1947 and 1958. The content of the letter makes 1947 the most plausible date. This is also the date that Schweber assumes to be correct.
- 8.
- 9.
Dirac Equation a (folio 1 (page 1)).
- 10.
Dirac Equation a (folio 1 (page 1)).
- 11.
Dirac Equation a, folio 2 (page 2), see Fig. 4.11, emph. in the original.
- 12.
Dirac Equation a, folio 3 (page 3), see Fig. 4.12.
- 13.
- 14.
- 15.
Dirac Equation a, folio 14 (page 12).
- 16.
Dirac Equation a, folio 11 (page 10).
- 17.
Dirac Equation a, folio 12 (page 11).
- 18.
RMP48, p. 367.
- 19.
Dirac Equation a, folio 12 (page 11).
- 20.
Dirac (1935).
- 21.
- 22.
Welton (2007, p. 46).
- 23.
Dirac (1946).
- 24.
- 25.
Dirac Equation a, folio 12 (page 11), emph. in the original.
- 26.
Dirac Equation a, folio 16 (page 13, last page) see Fig. 4.18.
- 27.
See, e. g., Dirac (1935, p. 270ff).
- 28.
- 29.
In other words: let \(\chi_{AB}=ab\), where a contains the factors that correspond to the extremal turns and b the factors that correspond to the left/right turns. If each factor were replaced with its complex conjugate we would have \(\chi_{BA}=\chi_{BA}^{*}=a^{*}b^{*}\). Now, because the factors that correspond to the extremal turns are, in fact, not replaced with their complex conjugates, we have instead \(\chi_{BA}=ab^{*}=\frac{ab^{*}}{a^{*}b^{*}}a^{*}b^{*}\). Since a is a product of an odd number of is, we have \(a={\mathrm{e}}^{{\mathrm{i}}\frac{\pi}{2}(2n+1)}\), where n is an integer, and, therefore, \(\chi_{BA}={\mathrm{e}}^{{\mathrm{i}}\pi(2n+1)}a^{*}b^{*}=-\chi_{AB}^{*}\).
- 30.
- 31.
Feynman (2005, p. 5).
- 32.
Feynman (2005, p. 31).
- 33.
See Wheeler and Feynman (1949, p. 425).
- 34.
- 35.
Feynman (2005, p. 10).
References
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Wüthrich, A. (2010). The Dirac Equation: Feynman’s Great Struggle. In: The Genesis of Feynman Diagrams. Archimedes, vol 26. Springer, Dordrecht. https://doi.org/10.1007/978-90-481-9228-1_4
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