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Propensity Interpretations

A propensity is a physical tendency: a disposition of a concrete setup to produce an outcome, present in the individual case whether or not the setup is ever repeated. On this interpretation, that a nucleus has probability of decaying within its half-life is a fact about that nucleus — as much a property of it as its mass — and not a fact about a sequence, a class, or anybody's beliefs.

Popper introduced the view in the 1950s for a specific reason: quantum mechanics assigns probabilities to single events, and frequentism cannot make sense of single-case probability. If the Born rule gives the chance that this atom decays now, and if that chance is a genuine physical fact, then probability must be capable of attaching to individuals. Propensity is the interpretation designed to let it.

This page distinguishes the long-run and single-case versions, sets out what recommends the view, and then examines the two objections that dominate the literature: that "propensity" merely names the explanandum, and that propensities — being causal and directed — cannot obey a calculus that is symmetric under inversion.


Two versions

Long-run propensity. A propensity is a disposition of a repeatable experimental arrangement to produce outcomes with a certain limiting frequency. The propensity belongs to the setup — the coin plus the tossing device plus the conditions — rather than to any individual trial. Popper's earlier formulation and Gillies's developed version take this line.

This is close to hypothetical frequentism, and deliberately so: it supplies the ground of the hypothetical frequency that frequentism has to posit without explanation. Where a frequentist says the probability is what the frequency would converge to, the long-run propensity theorist says it is the physical disposition in virtue of which it would converge, which answers the natural question of why the counterfactual has a determinate truth value.

The cost is that it does not solve the problem it was introduced for. If the propensity belongs to the arrangement rather than to the trial, then a genuinely unrepeatable event — the decay of this particular nucleus, or the outcome of a unique historical situation — still has no propensity of its own.

Single-case propensity. A propensity is a disposition of the individual case, given its complete physical state. This is Popper's later view and the one Giere and Fetzer develop. It delivers exactly what was wanted: a probability for the individual event, with the long-run frequency an effect of many trials with similar propensities rather than the definition of one.

Everything distinctive about the interpretation, and every serious problem, belongs to this version.

What recommends it

It takes physics at face value. In quantum mechanics probabilities appear in the fundamental dynamics, attached to individual systems, and are not obviously reducible to anything else. A decay probability is not a summary of a class — the nucleus does not consult a reference class before decaying — and is not plausibly a fact about our ignorance, since (on standard interpretations) there is no further fact to be ignorant of. Propensity is the interpretation that reads the theory literally.

It handles the single case and the reference class. Both problems that sink frequentism are solved at a stroke: the probability belongs to the concrete situation with all its properties, so there is no class to select and no question of which description to use. This is a genuine advantage and the reason the view persists despite the objections below.

It fits a broader metaphysics. Propensities are a species of disposition, and dispositional realism is an independently motivated position. On a powers ontology, fundamental properties just are dispositions to produce effects, and probabilistic dispositions are then no more mysterious than deterministic ones — a radium atom's tendency to decay differs only in degree from a charge's tendency to attract. An interpretation of probability that comes free with a metaphysics one holds anyway is attractive.

It explains why frequencies are evidence. Since propensities produce frequencies, observed frequencies are the natural evidence for propensities, and the law of large numbers is the theorem connecting them. The evidential role of statistics is preserved without the identification that causes frequentism its trouble.

The objections

"Propensity" names the problem

The most common complaint is that the interpretation is empty. Told that the coin has a propensity of to land heads, we ask what that consists in, and the only available answers are that it would produce heads about half the time in a long run — which is frequentism again — or that it is a primitive physical fact admitting no further analysis.

The second answer is not obviously illegitimate; every theory has primitives, and there is no rule that probability must be reducible to something non-probabilistic. But it does mean the interpretation is less informative than it appears. It relocates the mystery rather than dispelling it, and this is the same pattern the classical interpretation exhibits with equipossibility. The reply available to the propensity theorist is that a primitive with a clear role in physical explanation is in better standing than one with no role, and that dispositional properties are ubiquitous in science.

There is also an ascertainability worry. If the propensity of the individual case depends on its complete physical state, and two apparently similar setups can differ in propensity, then we can never be confident that our statistics are estimating the propensity we care about rather than an average over heterogeneous cases. The theory's metaphysical strength — attaching probability to the fully specific situation — is an epistemic weakness.

Humphreys' paradox

The sharpest technical objection, due to Paul Humphreys (1985), is that propensities cannot satisfy the probability calculus. The argument turns on asymmetry.

Probabilities invert freely. Given , Bayes' theorem yields

and both quantities are perfectly well defined probabilities. But propensities are causal tendencies, and causation is asymmetric. A photon's propensity to be transmitted by a filter is a genuine physical tendency; the "propensity" of a transmitted photon to have been emitted by a particular source is not a tendency of anything at all — the emission has already happened, and nothing is being brought about. Yet the calculus generates a number for it.

So either propensities do not obey the calculus — in which case they are not an interpretation of probability — or there exist inverse propensities, which appear to be causal tendencies running backwards in time. Neither horn is comfortable.

Responses fall into three groups, and none commands agreement.

  • Deny that propensities must be conditional probabilities. Treat propensity as attaching to unconditional single-case chances, with conditional probabilities defined from them in the ordinary way. This blunts the paradox, at the cost of making it unclear what the propensity is a propensity of, since dispositions are naturally relative to a triggering condition.
  • Accept the inverse quantities as probabilities but not as propensities. The calculus generates numbers that are legitimate degrees of belief without being tendencies. This is the most popular line, and it concedes something important: the propensity interpretation covers only part of the probability calculus, and needs a credence-based reading for the rest. That is pluralism, and it undercuts propensity's claim to be the interpretation of probability.
  • Restrict the domain. Hold that propensities are defined only for the forward-directed conditionals, treating the inverse as a formal artifact. This is coherent but concedes that "propensity" and "probability" are not co-extensive.

Humphreys himself drew the strong conclusion: probability theory is simply the wrong formalism for causal tendencies, and the attempt to interpret it propensity-wise should be abandoned rather than patched.

Determinism

If the world is deterministic, single-case propensities are trivial — every outcome has propensity or given the complete prior state. Yet statistical mechanics, population genetics, and actuarial science all use non-trivial probabilities, and they do not appear to be false.

The propensity theorist can say those probabilities are epistemic rather than physical, which is a coherent division of labour but concedes that propensity covers only fundamental-physical chance and nothing else. Since fundamental physics might turn out to be deterministic — Bohmian mechanics is empirically equivalent to standard quantum mechanics and fully deterministic — the interpretation risks having no application at all. Contrast the best-system account, which accommodates deterministic chance without strain, and see determinism and chance for the general question.

Assessment

CriterionVerdict
Admissibilitycontested — this is precisely what Humphreys' paradox denies
Ascertainabilityindirect only, via frequencies, with the heterogeneity worry above
Applicabilitystrong in fundamental physics, weak or absent elsewhere
Single casepasses — its reason for existing
Explains the calculuspoor — the calculus is imposed on propensities, not derived from them
Guidancegood, if the Principal Principle is granted — a known propensity plainly should guide belief

The profile is the mirror image of frequentism's. Frequentism explains the calculus and fails the single case; propensity passes the single case and struggles with the calculus. That complementarity is one of the better arguments for pluralism about probability.

Where this sits

Propensity is the most straightforwardly realist answer to the metaphysical question of the introduction: chances are physical properties of individual systems, as objective as masses. Its difficulties are the price of that realism, and they are all versions of one worry — that a directed causal tendency and a symmetric measure are different kinds of thing.

It is also the position most directly at stake in interpreting quantum mechanics. Whether the Born probabilities are propensities, frequencies, best-system chances, or degrees of belief is not settled by the formalism, and the mathematics of quantum probability — Gleason's theorem fixing the form of the measure without fixing its interpretation — is a further instance of the neutrality this section keeps returning to. The quantum chance page takes that up directly.

The next two pages cross to the epistemic side of the chance/credence divide, beginning with the position that dispenses with objective chance altogether: subjective Bayesianism.