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420<br />

new appendices<br />

to be slightly amended: in (ii) and in (v), we must replace ± 1 by ± ∞;<br />

and (iii) becomes:<br />

(iii)<br />

(1)<br />

0 � C(x, xy) = C(x, x) = C(x) =−log 2P(x) � +∞.<br />

The other desiderata remain as they were.<br />

Dr. Hamblin suggests 4 that we define degree of confirmation by<br />

C(x, y) = log 2(P(xy)/P(x)P(y))<br />

which for finite systems, but not necessarily for infinite systems, is the<br />

same as<br />

(2)<br />

C(x, y) = log 2(P(y, x)/P(y)),<br />

a formula which has the advantage of remaining determinate even if<br />

P(x) = 0, as may be the case if x is a universal theory. The corresponding<br />

relativized formula would be<br />

(3)<br />

C(x, y, z) = log 2(P(y, xz)/P(y, z)).<br />

The definition (1) does not, however, satisfy my desideratum viii (c),<br />

as Dr. Hamblin observes; and the same holds for (2) and (3). Desiderata<br />

ix (b) and (c) are also not satisfied.<br />

Now my desideratum viii (c) marks, in my opinion, the difference<br />

between a measure of explanatory power and one of confirmation. The<br />

former may be symmetrical in x and y, the latter not. For let y follow<br />

from x (and support x) and let x be unconfirmed by y. In this case it<br />

does not seem satisfactory to say that ax is always as well confirmed by y<br />

as is x. (But there does not seem to be any reason why ax and x should<br />

not have the same explanatory power with respect to y, since y is<br />

completely explained by both.) This is why I feel that viii(c) should not<br />

be dropped.<br />

4 C. L. Hamblin, op. cit., p. 83. A similar suggestion (without, however, specifying 2 as<br />

basis of the logarithm) is made in Dr. I. J. Good’s review of my ‘Degree of Confirmation’;<br />

cf. Mathematical Review, 16, 1955, 376.

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