Bourbaki

Theorem 3

Tag 03P5, permanent. Cite it as [Bourbaki, Tag 03P5].

Theory of Sets, chapter I, § 5. Equalitarian theories

((x=y) and (y=z))⇒(x=z)((x = y) \text{ and } (y = z)) \Rightarrow (x = z).

Let us adjoin the hypotheses x=yx = y, y=zy = z to the axioms of T0\mathscr{T}_0. By S6 the relation (x=y)⇒((x=z)⇔(y=z))(x = y) \Rightarrow ((x = z) \Leftrightarrow (y = z)) is true. Hence

(x=z)⇔(y=z),(x = z) \Leftrightarrow (y = z),

and consequently x=zx = z, are true.

C44. Let xx be a letter and let TT, UU, V{x}V\{x\} be terms in T0\mathscr{T}_0. Then the relation (T=U)⇒(V{T}=V{U})(T = U) \Rightarrow (V\{T\} = V\{U\}) is a theorem in T0\mathscr{T}_0.

For let yy and zz be two distinct letters which are distinct from xx and from the letters which appear in TT, UU, VV. Adjoin the hypothesis y=zy = z. Then, by S6,

((Y∣z)(V{y}=V{z}))⇔(V{y}=V{z}),((Y|z)(V\{y\} = V\{z\})) \Leftrightarrow (V\{y\} = V\{z\}),

that is to say (V{y}=V{y})⇔(V{y}=V{z})(V\{y\} = V\{y\}) \Leftrightarrow (V\{y\} = V\{z\}), is true. Now, V{y}=V{y}V\{y\} = V\{y\} is true by Theorem 1; hence V{y}=V{z}V\{y\} = V\{z\} is true.

From all this it follows that (y=z)⇒(V{y}=V{z})(y = z) \Rightarrow (V\{y\} = V\{z\}) is a theorem in T0\mathscr{T}_0, say AA. But (T∣y)(U∣z)A(T|y)(U|z)A is precisely

(T=U)⇒(V{T}=V{U}).(T = U) \Rightarrow (V\{T\} = V\{U\}).

¶ A relation of the form T=UT = U, where TT and UU are terms in T\mathscr{T}, is called an equation; a solution (in T\mathscr{T}) of the relation T=UT = U, considered as an equation in a letter xx, is therefore (§2, no. 2) a term VV in T\mathscr{T} such that T{V}=U{V}T\{V\} = U\{V\} is a theorem in T\mathscr{T}.

¶ Let TT and UU be two terms in T\mathscr{T}, and let x1x_1, x2x_2, ..., xnx_n be the letters which appear in TT but not in UU. If the relation

(∃x1)…(∃xn)(T=U)(\exists x_1)\ldots(\exists x_n)(T = U)

is a theorem in T\mathscr{T}, we say that U can be put in the form TT (in T\mathscr{T}). Let RR be a relation in T\mathscr{T} and let yy be a letter. Let VV be a solution (in T\mathscr{T}) of RR, considered as a relation in yy. If every solution (in T\mathscr{T}) of RR, considered as a relation in yy, can be put in the form VV, then VV is said to be the complete solution (or general solution) of RR (in T\mathscr{T}).

Bourbaki sets the proof directly after the statement, and the corpus does not separate them, so what is above is the statement and its proof together.

Cited by

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Cites

Transcribed from the printed edition, 2004, Springer. Not translated.