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Generalised Reichenbachian common cause systems

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Abstract

The principle of the common cause claims that if an improbable coincidence has occurred, there must exist a common cause. This is generally taken to mean that positive correlations between non-causally related events should disappear when conditioning on the action of some underlying common cause. The extended interpretation of the principle, by contrast, urges that common causes should be called for in order to explain positive deviations between the estimated correlation of two events and the expected value of their correlation. The aim of this paper is to provide the extended reading of the principle with a general probabilistic model, capturing the simultaneous action of a system of multiple common causes. To this end, two distinct models are elaborated, and the necessary and sufficient conditions for their existence are determined.

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Notes

  1. The existence of common causes in general or quantum probability spaces has been investigated by Gyenis and Rédei (2014, 2016), Kitajima (2008), and Kitajima and Rédei (2015). Whether, and under what conditions, the generalised models here proposed exist in such spaces will be left as an open question.

  2. Or, more exactly, any finite or countable number: in fact, no uncountable set of disjoint and non-zero probability events can exist given a countably additive probability measure (Wroński and Marczyk 2010). Thanks to an anonymous reviewer for pointing this out.

  3. For the existence of HR-RCCS of countably infinite size, see Marczyk and Wroński (2015).

References

  • Arntzenius, F. (1992). The common cause principle. In PSA: Proceedings of the biennial meeting of the philosophy of science association. Volume Two: Symposia and invited papers (pp. 227–237).

    Google Scholar 

  • Cartwright, N. (1979). Causal laws and effective strategies. Noûs, 13, 419–437.

    Article  Google Scholar 

  • Cartwright, N. (1988). How to tell a common cause: Generalizations of the common cause criterion. In J. H. Fetzer (Ed.), Probability and causality (pp. 181–188). Dordrecht: Reidel.

    Chapter  Google Scholar 

  • Cartwright, N. (1999). Causal diversity and the Markov condition. Synthese, 121, 3–27.

    Article  Google Scholar 

  • Eells, E. (1991). Probabilistic causality. Cambridge: Cambridge University Press.

    Book  Google Scholar 

  • Good, I. J. (1961). A causal calculus I. British Journal for the Philosophy of Science, 11, 305–318.

    Article  Google Scholar 

  • Graßhoff, G., Portmann, S., & Wuthrich, A. (2006). Minimal assumption derivation of a Bell-type inequality. The British Journal for the Philosophy of Science, 56, 663–680.

    Article  Google Scholar 

  • Gyenis, Z., & Rédei, M. (2014). Atomicity and causal completeness. Erkenntnis, 79, 437–451.

    Article  Google Scholar 

  • Gyenis, Z., & Rédei, M. (2016). Common cause completability of non-classical probability spaces. Belgrade Philosophical Annual, 29, 15–32.

    Article  Google Scholar 

  • Hempel, C. (1965). Aspects of scientific explanation and other essays in philosophy of science. New York: Free Press.

    Google Scholar 

  • Hofer-Szabó, G., & Rédei, M. (2004). Reichenbachian common cause systems. International Journal of Theoretical Physics, 43, 1819–1826.

    Article  Google Scholar 

  • Hofer-Szabó, G., & Rédei, M. (2006). Reichenbachian common cause systems of arbitrary finite size exist. Foundations of Physics, 36, 745–756.

    Article  Google Scholar 

  • Hofer-Szabó, G., Rédei, M., & Szabó, L. E. (2013). The principle of the common cause. Cambridge: Cambridge University Press.

    Book  Google Scholar 

  • Kitajima, Y. (2008). Reichenbach’s common cause in an atomless and complete orthomodular lattice. International Journal of Theoretical Physics, 47, 511–519.

    Article  Google Scholar 

  • Kitajima, Y., & Rédei, M. (2015). Characterizing common cause closedness of quantum probability theories. Studies in the History and Philosophy of Modern Physics, 52(B), 234–241.

    Article  Google Scholar 

  • Marczyk, M., & Wroński, L. (2015). Completion of the causal completability problem. British Journal for the Philosophy of Science, 66, 307–326.

    Article  Google Scholar 

  • Mazzola, C. (2012). Reichenbachian common cause systems revisited. Foundations of Physics, 42, 512–523.

    Article  Google Scholar 

  • Mazzola, C. (2013). Correlations, deviations and expectations: The extended principle of the common cause. Synthese, 190, 2853–2866.

    Article  Google Scholar 

  • Mazzola, C., & Evans, P. (2017). Do Reichenbachian common cause systems of arbitrary finite size exist? Foundations of Physics, 47, 1543–1558.

    Article  Google Scholar 

  • Pearl, J. (1988). Probabilistic reasoning in intelligent systems. San Mateo: Morgan Kauffman.

    Google Scholar 

  • Pearl, J. (2000). Causality. Cambridge: Cambridge University Press.

    Google Scholar 

  • Reichenbach, H. (1956). The direction of time. Berkeley: University of California Press.

    Book  Google Scholar 

  • Salmon, W. C. (1971). Statistical explanation and statistical relevance. Pittsburgh: Pittsburgh University Press.

    Book  Google Scholar 

  • Salmon, W. C. (1984). Scientific explanation and the causal structure of the world. Princeton: Princeton University Press.

    Google Scholar 

  • Skyrms, B. (1980). Causal necessity. New Haven: Yale University Press.

    Google Scholar 

  • Sober, E. (1984). Common cause explanation. Philosophy of Science, 5, 212–241.

    Article  Google Scholar 

  • Spirtes, P., Glymour, C., & Scheines, R. (2001). Causation, prediction, and search (2nd ed.). Cambridge: MIT Press.

    Book  Google Scholar 

  • Stergiou, C. (2015). Explaining correlations by partitions. Foundations of Physics, 45, 1599–1612.

    Article  Google Scholar 

  • Suppes, P. (1970). A probabilistic theory of causality. Amsterdam: North-Holland Publishing Company.

    Google Scholar 

  • Suppes, P., & Zaniotti, M. (1981). When are probabilistic explanations possible? Synthese, 48, 191–199.

    Article  Google Scholar 

  • van Fraassen, B. (1980). The scientific image. Oxford: Clarendon Press.

  • van Fraassen, B. (1982). Rational belief and the common cause principle. In R. McLaughlin (Ed.), What? Where? When? Why? (pp. 193–209). Dordrecht: Reidel.

    Chapter  Google Scholar 

  • van Fraassen, B. (1991). Quantum mechanics: An empiricist view. Oxford: Clarendon Press.

  • Williamson, J. (2005). Bayesian nets and causality. Oxford: Oxford University Press.

    Google Scholar 

  • Wroński, L., & Marczyk, M. (2010). Only countable Reichenbachian common cause systems exist. Foundations of Physics, 40, 1155–1160.

    Article  Google Scholar 

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Acknowledgements

I am grateful to two anonymous referees for their challenging but constructive feedback.

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Correspondence to Claudio Mazzola.

Appendix: Proof of Lemma 5

Appendix: Proof of Lemma 5

Let \((\varOmega , p)\) be a classical probability space with \(\sigma \)-algebra of random events \(\varOmega \) and probability measure p. Moreover, let \(A,B\in \varOmega \) satisfy (17) and (62).

To start with, let us observe that (43) is in fact a system of \(n-1\) equations, namely one for each value of \(i = 1, \ldots , n-1\). Therefore, (39)–(43) jointly comprise a system of \(4 + (n - 1) = n + 3\) equations in 4n variables. This means that each HR-admissible set for \(\delta \left( {A},{B}\right) \) is determined by a set of \(4n - (n+3) = 3n- 3\) parameters, for every \(n\ge 2\). To establish the existence of such set, we accordingly need to prove that such parameters exist. To this purpose, let numbers a, b and \(\varepsilon \) be understood as per (44)–(46). Proof will proceed by induction on n.

Let us begin by assuming \(n = 2\) as our inductive basis. This has the effect of transforming (39)–(43), respectively, into:

$$\begin{aligned}&\displaystyle a_{2} = \frac{a - c_{1} a_{1}}{1-c_{1}} \end{aligned}$$
(89)
$$\begin{aligned}&\displaystyle b_{2} = \frac{b- c_{1} b_{1}}{1-c_{1}} \end{aligned}$$
(90)
$$\begin{aligned}&\displaystyle c_{2} = 1- c_{1} \end{aligned}$$
(91)
$$\begin{aligned}&\displaystyle d_{2} = \varepsilon + \frac{[a - a_{1}c_{1}][b - b_{1}c_{1}]}{[ 1 - c_{1}]^{2}} \end{aligned}$$
(92)
$$\begin{aligned}&\displaystyle d_{1} - a_{1}b_{1} = \varepsilon . \end{aligned}$$
(93)

Since a, b and \(\varepsilon \) are known by hypothesis, choosing numbers \(c_{1}\), \(a_{1}\) and \(b_{1}\) will therefore suffice to fix the values of all \(4n = 8\) variables in the system. In particular, (89)–(92) immediately produce:

$$\begin{aligned} lim_{c_{1}\rightarrow 0} \ a_{2}= & {} a \end{aligned}$$
(94)
$$\begin{aligned} lim_{c_{1}\rightarrow 0} \ b_{2}= & {} b \end{aligned}$$
(95)
$$\begin{aligned} lim_{c_{1}\rightarrow 0} \ c_{2}= & {} 1 \end{aligned}$$
(96)
$$\begin{aligned} lim_{c_{1}\rightarrow 0} \ d_{2}= & {} \varepsilon + ab, \end{aligned}$$
(97)

while on the other hand (17) directly requires that

$$\begin{aligned} 1> a,b > 0, \end{aligned}$$
(98)

as it would be easy to verify. Taken together this ensures that, as \(c_{1}\) is taken sufficiently close to zero:

$$\begin{aligned} 1\ge & {} a_{2}, b_{2} \ge 0 \end{aligned}$$
(99)
$$\begin{aligned} 1\ge & {} c_{1}, c_{2} \ge 0, \end{aligned}$$
(100)

while (62) and (17) imply that

$$\begin{aligned} 1 \ge d_{2} \ge 0. \end{aligned}$$
(101)

To determine the remaining numbers, we further need to set \(a_{1}\) and \(b_{1}\). In this case, our choice will depend on the value of \(\varepsilon \), as follows:

$$\begin{aligned} \varepsilon\ge & {} 0 \phantom {12 pt} {\left\{ \begin{array}{ll} a> a_{1} \ge 0\\ b > b_{1} \ge 0 \end{array}\right. } \end{aligned}$$
(102)
$$\begin{aligned} \varepsilon< & {} 0 \phantom {12 pt} {\left\{ \begin{array}{ll} 1 \ge a_{1}> a \\ 1 \ge b_{1} > b \end{array}\right. } \end{aligned}$$
(103)

Either option is allowed by (98), and either will ensure that

$$\begin{aligned} 1 \ge d_{i} \ge 0, \end{aligned}$$
(104)

as it would be straightforward to check with the aid of (43), (17) and (62). Thanks to Lemma 3, this is enough to establish that some set \(\left\{ {a_{i}, b_{i}, c_{i}, d_{i}}\right\} _{{i = 1}}^{{n}}\) of quasi-admissible numbers exist for \(\delta \left( {A},{B}\right) \) if \(n = 2\). To further show that such set is HR-admissible for \(\delta \left( {A},{B}\right) \), we only need to observe that (34) can be obtained from both (102) and (103), owing to (28)–(30).

Let us now assume, as our inductive hypothesis, that some set \(\left\{ {a_{i}, b_{i}, c_{i}, d_{i}}\right\} _{{i = 1}}^{{m}}\) is HR-admissible for \(\delta \left( {A},{B}\right) \), where \(n = m > 2\). To prove that a HR-admissible set for \(\delta \left( {A},{B}\right) \) also exists if \(n = m +1\), let us consider the set

$$\begin{aligned} \left\{ {a_{j}, b{j}, c_{j}, a_{m-1}, b_{m-1}}\right\} _{{j = 1}}^{{m-2}}\subset \left\{ {a_{i}, b_{i}, c_{i}, d_{i}}\right\} _{{i = 1}}^{{m}}, \end{aligned}$$

and let us choose numbers \(a'_{m} , b'_{m}, c'_{m-1}, c'_{m} \) such that:

$$\begin{aligned}&\displaystyle a_{j}> a'_{m} > 0 \phantom {12 pt} ( j = 1, \ldots , m-1) \end{aligned}$$
(105)
$$\begin{aligned}&\displaystyle b_{j}> b'_{m} > 0 \phantom {12 pt} ( j = 1, \ldots , m-1) \end{aligned}$$
(106)
$$\begin{aligned}&\displaystyle c_{m}, c_{m-1}> c'_{m-1} > 0 \end{aligned}$$
(107)
$$\begin{aligned}&\displaystyle 1> c'_{m} > 0. \end{aligned}$$
(108)

Given (39)–(43), the set

$$\begin{aligned} \left\{ {a_{j}, b{j}, c_{j}, a_{m-1}, b_{m-1}}\right\} _{{j = 1}}^{{m-2}}\cup \left\{ {a'_{m}, b'_{m}, c'_{m-1}, c'_{m}}\right\} _{{}}^{{}} \end{aligned}$$

of \(3n-3\) parameters will then suffice to determine \(4(m+1)\) numbers:

$$\begin{aligned} \left\{ {a_{j}, b_{j}, c_{j}, d_{j}, a_{m-1}, b_{m-1}, c'_{m-1}, d_{m-1}, a'_{m}, b'_{m}, c'_{m}, d'_{m}, a_{m+1}, b_{m+1}, c_{m+1}, d_{m+1}}\right\} _{{j = 1}}^{{m-2}}. \end{aligned}$$

Because numbers \(\left\{ {a_{j}, b_{j}, c_{j}, d_{j}, a_{m-1}, b_{m-1}, c'_{m-1}, d_{m-1}, a'_{m}, b'_{m}, c'_{m},}\right\} _{{j = 1}}^{{m-1}}\) satisfy conditions (31)–(33) and (34) by hypothesis, all we need to show is that said constraints are also satisfied by the remaining numbers \(\left\{ {d'_{m}, a_{m+1}, b_{m+1}, c_{m+1}, d_{m+1}}\right\} _{{}}^{{}}\). To this purpose, let us first notice that (32) must be true of \(d'_{m}\) by virtue of (43) and (105)–(106). Next, thanks to (39)–(42), it will be sufficient to suppose that

$$\begin{aligned}&a'_{m} \rightarrow 0 \end{aligned}$$
(109)
$$\begin{aligned}&b'_{m} \rightarrow 0 \end{aligned}$$
(110)
$$\begin{aligned}&c'_{m} \rightarrow c_{m-1}-c'_{m-1} \end{aligned}$$
(111)

to obtain

$$\begin{aligned}&lim_{a'_{m} \rightarrow 0, \ c'_{m} \rightarrow c_{m-1}-c'_{m-1}} a_{m+1} = a_{m} \end{aligned}$$
(112)
$$\begin{aligned}&lim_{b'_{m} \rightarrow 0, \ c'_{m} \rightarrow c_{m-1}-c'_{m-1}} b_{m+1} = b_{m} \end{aligned}$$
(113)
$$\begin{aligned}&lim_{c'_{m} \rightarrow c_{m-1}-c'_{m-1}} c_{m+1} = c_{m} \end{aligned}$$
(114)
$$\begin{aligned}&lim_{a'_{m} \rightarrow 0, \ b'_{m} \rightarrow 0, \ c'_{m} \rightarrow c_{m-1}-c'_{m-1}} d_{m+1} = d_{m} \end{aligned}$$
(115)

which we already know, by our inductive hypothesis, to satisfy (31)–(33). Moreover, (105) and (106), along with the inductive assumption whereby

$$\begin{aligned} {[}a_{m} - a_{i}][b_{m}-b_{i}] > 0 \phantom {12 pt} (i = 1, \ldots , m-1), \end{aligned}$$
(116)

ensures that

$$\begin{aligned} {[}a_{m+1} - a_{i}][b_{m+1}-b_{i}] > 0 \phantom {12 pt} (i = 1, \ldots , m), \end{aligned}$$
(117)

which together with our inductive hypothesis suffices to establish (34). Due to Lemma 3 and Definition 8, the set of \(4(m+1)\) numbers so determined is therefore HR-admissible for \(\delta \left( {A},{B}\right) \). Lemma 5 is thus demonstrated by induction.

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Mazzola, C. Generalised Reichenbachian common cause systems. Synthese 196, 4185–4209 (2019). https://doi.org/10.1007/s11229-017-1650-2

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