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popper-logic-scientific-discovery

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Our theorem has been derived by considering finite universes, and it<br />

is indeed quite independent of the transition to infinite universes. It is<br />

therefore independent of the formulae (1) and (2) of the preceding<br />

appendix, that is to say, of the fact that in an infinite universe, we have<br />

for any universal law a and any finite evidence e,<br />

(2)<br />

p(a) = p(a, e) = 0.<br />

We may therefore legitimately use (1) for another derivation of (2);<br />

and this can indeed be done, if we utilize an idea due to Dorothy<br />

Wrinch and Harold Jeffreys.<br />

As briefly indicated in the preceding appendix, 4 Wrinch and Jeffreys<br />

observed that if we have an infinity of mutually incompatible or<br />

exclusive explanatory theories, the sum of the probabilities of these<br />

theories cannot exceed unity, so that almost all of these probabilities<br />

must be zero, unless we can order the theories in a sequence, and<br />

assign to each, as its probability, a value from a convergent sequence of<br />

fractions whose sum does not exceed 1. For example, we may make the<br />

following assignments: we may assign the value 1/2 to the first theory,<br />

1/2 2 to the second, and, generally, 1/2 n to the nth. But we may also<br />

assign to each of the first 25 theories the value 1/50, that is to say,<br />

1/(2.25); to each of the next 100, say, the value 1/400, that is to<br />

say, 1/(2 2 .100) and so on.<br />

However we may construct the order of the theories and however we<br />

may assign our probabilities to them, there will always be some greatest<br />

probability value, P say (such as 1/2 in our first example, or 1/50), and<br />

this value P will be assigned to at most n theories (where n is a finite<br />

number, and n.P < 1). Each of these n theories to which the maximum<br />

probability P has been assigned, has a dimension. Let D be the largest<br />

dimension present among these n theories, and let a 1 be one of them,<br />

with d(a 1) = D. Then, clearly, none of the theories with dimensions<br />

greater than D will be among our n theories with maximum probability.<br />

Let a 2 be a theory with a dimension greater than D, so that<br />

d(a 2)>D = d(a 1). Then the assignment leads to:<br />

4 Cf. appendix *vii, text to footnote 11.<br />

appendix *viii 397

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