Abstract
Einstein and Hilbert both struggled to reconcile general covariance and causality in their early work on general relativity. In Einstein’s case, this first led to his infamous “hole argument”, a stumbling block that persuaded him early on that generally covariant field equations for gravitation could never be found. After his breakthrough to general covariance in the fall of 1915, the resolution came in form of the “point-coincidence argument.” Hilbert from the beginning took a different view of the “causality problem,” though he shifted his position somewhat in the light of Einstein’s breakthrough in November 1915. Nevertheless, his aim was to establish initial conditions that would lead to a well-defined Cauchy problem in general relativity. Hilbert consistently advocated the use of coordinate conditions in order to obtain solutions of the field equations that would maintain the causal ordering of events. Einstein’s “causality problem” thus differs from that of Hilbert, and the latter was never a victim of Einstein’s “hole argument.”
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Notes
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- 2.
For more on Einstein’s (mis)appropriation of Mach’s principle, see Barbour (2005).
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The “December Proofs” (Hilbert 1915a) were recently discovered (see Corry, L., J. Renn, and J. Stachel (1997) and contain significant differences from the published version (Hilbert 1915b). For discussion of these differences, and differing opinions on their significance, see Renn and Stachel (1999), and Sauer (1999, 2005).
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Some commentators have mistakenly asserted that Hilbert’s equations are not generally covariant. On this issue we wholeheartedly support Ohanian’s recent statement when he writes: “The fact is that Hilbert’s variational equations are covariant, but he supplements them, correctly, by extra, noncovariant, coordinate conditions that are needed to make the solution unique, as is well known to anybody who has ever tried to construct a solution of the Einstein equations.” (Ohanian 2008, p. 355 (n. 56 to p. 221)).
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See, once again, Ohanian (2008, n. 56), cited above.
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Indeed, to go further, Hilbert’s epistemological analysis of the differing status that should be accorded to general covariance versus causality might perhaps be suggestive to those working on the interpretation of General Relativity as a gauge theory, and the associated “problem of time” in quantum gravity.
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Stachel (1992) writes that while Einstein was “always a bit vague about just what he meant by causality” in his hole argument, Hilbert on the other hand “gave a quite precise meaning to the concept”, formulating it in the context of whether the field equations can be expressed in Cauchy normal form. Surely it is right that Hilbert was led to think about causality in the context of general covariance by Einstein’s concerns in the summer of 1915, and Stachel is of course exactly right that Hilbert’s version of the problem is stated in the precise mathematical language of the Cauchy problem. What we wish to emphasize is that the problem Hilbert thus arrives at is importantly different from that with which Einstein wrestled in his hole argument.
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See section on Hilbert’s causality problem, above.
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Brading, K., Ryckman, T. (2018). Hilbert on General Covariance and Causality. In: Rowe, D., Sauer, T., Walter, S. (eds) Beyond Einstein. Einstein Studies, vol 14. Birkhäuser, New York, NY. https://doi.org/10.1007/978-1-4939-7708-6_3
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