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338<br />

new appendices<br />

The following comments may be made upon this system of<br />

postulates:<br />

The six axioms—A1, A2, A3, B1, B2, and B3—are explicitly used<br />

in the actual operations of deriving the theorems. The remaining<br />

(existential) parts of the postulates can be taken for granted, as in the<br />

paper in which I first published this system of axioms. (Cf. note 1,<br />

above.)<br />

At the price of introducing a fourth variable, ‘d’, in Postulates 3 and<br />

4, these six axioms may be replaced by a system of only four axioms,<br />

consisting of A1, A2, and the following two:<br />

B If p(a, bc)p(b, c) ≠ p(d, c) provided that p(a, c) � p(d, c), then<br />

+<br />

p(ab, c) ≠ p(d, c)<br />

C If p(a, b) + p(ā, b) ≠ p(c, c) then p(c, c) = p(d, b)<br />

+<br />

In this system, B + is equivalent to the conjunction of B1 and B2, and<br />

This system looks very much like some of the customary systems (except for the omission<br />

of antecedents in the axioms other than C′, and the form of the antecedent of C′);<br />

and it is remarkable that it yields for the elements a, b, . . . , as does the system in the text,<br />

the theorems of Boolean algebra which ordinarily are separately assumed. Nevertheless it<br />

is unnecessarily strong; not only because it introduces the numbers 1 and 0 (thus hiding<br />

the fact that these need not be mentioned in the axioms) but also because A3, B1, and<br />

C follow immediately from A3′, A4′, and C′, while for the opposite derivations, all<br />

the axioms of the system given in the text except A2 are indispensable. (For these<br />

derivations, see appendix *v.)<br />

Within the system of axioms here described, and also within the system given in<br />

the text, the conjunction of the axioms A4′ and B1′ is replaceable by B1, and vice<br />

versa. My independence proofs (given below) are applicable to the system here<br />

described.<br />

The derivation of B1 from A4′ and B1′, in the presence of the axioms A3 or A3′, C or<br />

C′, and B2, is as follows:<br />

(1) 0 � p(a, b) � p(a, a) A4′; C or C′; A3 or A3′<br />

(2) p(a, a) � p((aa)a, a) = p(aa, aa)p(a, a) = p(a, a) 2 1, A3′; B2; A3 or A3′<br />

(3) 0 � p(a, b) � p(a, a) � 1 1, 2<br />

(4) p(ba, c) � p(a, c) B2, 3<br />

Now we apply B1′<br />

(5) p(ab, c) � p(a, c) 4. B1′<br />

For the derivation of A4′ and B1′ from B1, see appendix *v.

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