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224<br />

some structural components of a theory of experience<br />

be regarded as a decisive argument, as a kind of experimentum crucis, in<br />

favour of the statistical interpretation of the quantum theory.<br />

76 AN ATTEMPT TO ELIMINATE METAPHYSICAL<br />

ELEMENTS BY INVERTING HEISENBERG’S<br />

PROGRAMME; WITH APPLICATIONS<br />

If we start from the assumption that the formulae which are peculiar to<br />

quantum theory are probability hypotheses, and thus statistical statements,<br />

then it is difficult to see how prohibitions of single events could<br />

be deduced from a statistical theory of this character (except perhaps in<br />

the cases of probabilities equal to one or to zero). The belief that single<br />

measurements can contradict the formulae of quantum physics seems<br />

<strong>logic</strong>ally untenable; just as untenable as the belief that a contradiction<br />

might one day be detected between a formally singular probability<br />

statement αP k(β) = p (say, ‘the probability that the throw k will be a five<br />

equals 1/6’) and one of the following two statements: k εβ (‘the throw<br />

is in fact a five’) or k εβ - (‘the throw is in fact not a five’).<br />

These simple considerations provide us with the means of refute any<br />

of the alleged proofs which have been designed to show that exact<br />

measurements of position and momentum would contradict the quantum<br />

theory; or which have been designed, perhaps, to show that the<br />

mere assumption that any such measurements are physically possible<br />

must lead to contradictions within the theory. For any such proof must<br />

make use of quantum-theoretical considerations applied to single particles;<br />

which means that it has to make use of formally singular probability<br />

statements, and further, that it must be possible to translate the<br />

proof—word for word, as it were—into the statistical language. If we<br />

do this then we find that there is no contradiction between the single<br />

measurements which are assumed to be precise, and the quantum<br />

theory in its statistical interpretation. There is only an apparent contradiction<br />

between these precise measurements and certain formally singular<br />

probability statements of the theory. (In appendix v an example<br />

of this type of proof will be examined.)<br />

But whilst it is wrong to say that the quantum theory rules out exact<br />

measurements, it is yet correct to say that from formulae which are<br />

peculiar to the quantum theory—provided they are interpreted

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