Abstract
Howson famously argues that the no-miracles argument, stating that the success of science indicates the approximate truth of scientific theories, is a base rate fallacy: it neglects the possibility of an overall low rate of true scientific theories. Recently a number of authors has suggested that the corresponding probabilistic reconstruction is unjust, as it concerns only the success of one isolated theory. Dawid and Hartmann, in particular, suggest to use the frequency of success in some field of research \(\mathcal {R}\) to infer a probability of truth for a new theory from \(\mathcal {R}\). I here shed doubts on the justification of this and similar moves and suggest a way to directly bound the probability of truth. As I will demonstrate, my bound can become incompatible with the assumption specific testing and Dawid and Hartmann’s estimate for success.
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02 March 2020
An argument against global no miracles
Notes
My notation will diverge from DH’s, but it should always be entirely clear what is meant.
I will be quite liberal on counting one theory as the ‘limit’ of another, thus allowing for all kinds of adaptive strategies; e.g. when one arises from the introduction of new fundamental parameters into the other or when one is a quantization of the other, in which case the scope and meaning of limits such as \(\hbar \rightarrow 0\) becomes especially delicate (cf. Ballentine 2000, pp. 388–389). It should be noted that this is a concession to the NMA defendant.
If you are at unease with this move, e.g. for the problems of uncertain or old evidence (cf. Talbott 2008, §6.2), you may replace ‘informed prior’ by ‘posterior’ in all following instances. Nothing really depends on this terminological choice.
While immediate, a proof of (6) is provided in the “Appendix”, for completeness’ sake.
I am hence not advocating a version of Laudan’s (1984) pessimistic meta-induction here. The same holds for the next section, where incompatible theories are considered that persist together.
I should also mention Sprenger’s (2016) reconstruction of the NMA in this connection. Among other things, Sprenger (pp. 174–175) suggests that the NMA can be weakened to concern only empirical adequacy. But the NMA has been the pivotal argument for ‘full blown’ scientific realism(s), and what is observable (say) in quantum theories, at least in van Fraassen’s (1980, p. 16) narrow sense, is arguably just the behavior of ‘macroscopic measuring devices’. If quantum theories are interpreted as being mostly concerned with the behavior of microscopic particles, global wavefunctions, or the like, their empirical adequacy thus means far less than their approximate truth.
Morrison (2011) also provides a detailed analysis of nuclear physics as a domain of science where rivaling paradigms are not merely complementary but mutually contradicting. I will reference some of her findings below.
The notion ‘model’ should not divert us from the main subject here. Cook (2010, p. 57), for instance, has it that “‘theory’, [...] and ‘model’, are often used loosely to mean the same thing”, and Hartmann (1996, p. 80) observes that “[b]y and large, scientists prefer ‘model’, because [...] it is safer to label one’s thought products ‘models’ instead of ‘theories’ for they are most likely provisionary anyway [...].”
Recall that the surface area of a sphere of radius \(R_{0}\) is \(4\pi R_{0}^{2}\); this and the relation between \(R_{0}\) and \(A^{1/3}\) briefly discussed below explains the \(A^{2/3}\) dependency.
In analogy to the magnetic quantum number \(m_{\ell }\) or the spin projection \(m_{s}\) in atomic and particle physics, there is a projection in the nuclear shell model. When each of the values of \(\Omega \) for a given j is taken on by some nucleon, the corresponding j-shell is called closed. Whenever there is a large energy gap between two sets of energy levels, which usually occurs between a closed shell and the next unfilled one, this is called a major shell closure and the number of nucleons in all the shells occupied up to that point is called ‘magic’ (cf. Greiner and Maruhn 1996, p. 245).
The delta-function potential can hence be understood as an idealized representation of an extremely short-range interaction.
Note that this immediately sheds doubt on Menke’s (2014, p. 106) claim that to defend the NMA against the BRF, “it is important to distinguish between theories that have made one successful prediction and theories that made two or even more, and not to regard them on a par with each other.”
Cf. also Morrison (2011, pp. 350–351) on this point.
An anonymous referee has confronted me with the suggestion that a realist might take those (structural) elements for real that are used in the derivation of the relevant predictions. As the discussion should have shown, this would amount to embracing outright inconsistencies, as fundamental assumptions that are in contradiction with one another (e.g. strong vs. negligible interaction between nuclei) are necessary to get the predictions. Hence like Morrison (2011, p. 351) I believe that “this is not a situation that is resolvable using strategies like partial structures[...].”
I here also rely on mentions of explanation of experimental knowledge by some model in Greiner and Maruhn’s book, since the explanations in this context are of the deductive-nomological kind. The term, in other words, means nothing but the (non-trivial) derivation of experimental facts from the ‘nomoi’ of the respective model, which amounts to a (use-)novel prediction, as I have detailed in Sect. 2.1.
I hence now assume an equality in my adapted (ii*) again, for ease of computation. In case you are uncomfortable with this back and forth, just replace \(f\mapsto f'\) in what follows, where \( p(s|\lnot t, \hat{s} \& \hat{c})=f'<f\).
I should dispel a potential distraction here. DH (p. 11), namely, demonstrate that n / m need not be too high for their argument to work. The (approximate) lower bound they derive is \(n/m>2p(s|\lnot t, \hat{s})\), which is typically still \(\ll 1\) on account of (ii*). But of course a higher success rate, if allowed as a success estimate for new theories, would displace the NMA even further from the danger of becoming a BRF. My example demonstrates that there are domains where n / m happens to exceed this lower bound by far, so long as (ii*) is accepted, but the assignment of a sufficiently high probability for truth may be forestalled by consistency anyways.
The reader will again appreciate the obvious similarity to Henderson (2017).
They imply incompatible ontologies, they do not all share the same dynamics, and some of them even rely on quite different (additional) formal methods than others. Cf. also Boge (2018) for an overview.
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Acknowledgements
I thank Florian Fischer for getting me interested in the base rate fallacy, Michael Stöltzner for critical input at an earlier stage, Radin Dardashti for helpful advice on references and some discussion on the subject, and a number of anonymous referees for helpful comments on earlier versions.
Funding
A significant part of the research for this paper was conducted during my employment with the research unit The Epistemology of the Large Hadron Collider, funded by the German Research Foundation (DFG) (Grant FOR 2063).
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Appendix
Appendix
We here quickly prove eqn. (6). For simplicity, we write \( \tilde{p}(x)\equiv p(x|\hat{s} \& \hat{c})\) for any x below. From (5), the adapted versions of (i*) and (ii*), and (\(*\)), we have
Now assume that \(\tilde{p}(s)\) is greater or equal to \(g/k+f\). Then we have
which implies
Contradiction. \(\square \)
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Boge, F.J. An argument against global no miracles arguments. Synthese 197, 4341–4363 (2020). https://doi.org/10.1007/s11229-018-01925-9
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DOI: https://doi.org/10.1007/s11229-018-01925-9