Abstract
Structural realists claim that structure is preserved across instances of radical theory change, and that this preservation provides an argument in favor of realism about structure. In this paper, I use the shift from Newtonian gravity to Einstein’s general relativity as a case study for structural preservation, and I demonstrate that two prominent views of structural preservation fail to provide a solid basis for realism about structure. The case study demonstrates that (i) structural realists must be epistemically precise about the concrete structure that is being preserved, and (ii) they must provide a metaphysical account of how structure is preserved through re-interpretation in light of a new theory. Regarding (i), I describe a means of epistemic access to the unobservable that I call “thick detection” of structure, which isolates the structure that will be preserved. Regarding (ii), I argue that thickly detectable structure is preserved across theory change through a process of extracting the old structure from the new structure, much like what has been done with geometrized versions of Newtonian gravity. With these two responses in hand, the structural realist can adequately account for the preservation of structure and can provide a strong argument in favor of structural realism.
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Notes
See Ladyman and Ross (2007) and French (2014) for defenses of ontic structural realism. See Votsis (2003), Morganti (2004), and Hanson-Park (2023) for defenses of epistemic structural realism. Lastly, see Ladyman (2021) for an argument that structural realism is not properly a form of selective realism, as I treat it in this paper.
The details of the equivalence principle are not essential for demonstrating the preservation of structural elements in the case study at hand. For more on the equivalence principle, see Einstein (1961: chapters 19–20), Poisson and Will (2014: 218–221), and Adler (2021: Section 7.2) for the physics, or see Rohrlich (2000) and Lehmkuhl (2021) for the philosophical implications.
To be precise, Worrall is appropriating Post’s (1971) “principle of general correspondence,” which involves the laws in the new theory “degenerating” into the laws of the old given the right limiting conditions.
Note that this is not to say that Ptolemy was a realist about epicycles. Instead, this may be a structural claim of Ptolemy’s theory according to the structural realist, and the structural realist must explain this in light of its falsity. For a different structuralist account of the similarities between Ptolemaic and Copernican astronomy not based on thick detection, see Saunders (1993).
For the sake of brevity, hereafter I will speak of the terms themselves being detectable rather than making the more metaphysically accurate but linguistically cumbersome statement that the properties represented by the terms are detectable.
I take measurement (as distinct from mere calculation) to be a form of detection, so anything that is measurable is detectable. However, it is not necessarily the case that anything measurable is thickly detectable, as I will discuss in Section 6. Since no gravitational force exists in reality, it is the magnitude of this ‘force’ that is detectable. This will also be clarified in Section 6.
As Knox (2014) argues, GNG may be preferable on Newton’s own terms, had he considered it.
One may worry that I am making structural realism vulnerable to Stanford’s (2006) problem of unconceived alternatives with this claim, but this is not the case. In short, it is my view that if scientists fail to satisfy the robustness criterion, this takes thick detection off the table but not truth or abductive justification.
For a further explanation of this event, see CERN’s press release (https://home.cern/news/press-release/cern/opera-experiment-reports-anomaly-flight-time-neutrinos-cern-gran-sasso) and Antonello et al. (2012).
See Melia and Saatsi (2006) for more details on how the structural realist can have higher-order knowledge of relations between first-order predicates. There are many forms this higher-order knowledge can take, and each of these instances will be another instance of structure about which we should be realists, but discussing this is in further detail does not advance the case of structural preservation that I am making here.
Remember that I take measurement to be a form of detection, and measurable properties are thickly detectable only if they satisfy the three criteria from Section 6.
In this paragraph, I make use of the very helpful explanations in Cheng (2005) of each of the terms in the Einstein field equations. Cheng’s explanations are standard, so nothing I say will stand or fall based on his account of the mathematics involved.
To be clear, the physical distances being represented by the Ricci curvature tensor and the scalar curvature are not themselves directly measurable. Instead, these are representations of the distances in a curved, pseudo-Riemannian metric. Since these representations can be detected by the phenomena predicted by general relativity (such as the motion of particles and the bending of light) and the detection of these phenomena are robust, refinable, and connectable, they satisfy the criteria for thick detection that I have set out in this paper.
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Acknowledgements
Thanks to Berit Brogaard, Otávio Bueno, Anjan Chakravartty, Steven French, Kari Hanson-Park, Shea Musgrave, Hwan Ryu, Ziren Yang, and the anonymous reviewers for comments and discussion that have greatly improved this paper.
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Hanson-Park, J. The preservation of thickly detectable structure: a case study in gravity. Euro Jnl Phil Sci 14, 27 (2024). https://doi.org/10.1007/s13194-024-00588-3
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DOI: https://doi.org/10.1007/s13194-024-00588-3