Field axioms are numbered as in Field and the two order axioms as in Ordered Field. The order is a total order, hence reflexive, transitive, antisymmetric and total.
We first record two field identities. For every cβF we have cβ
0=0: by axioms 2 and 9, cβ
0=c(0+0)=cβ
0+cβ
0, and adding the additive inverse of cβ
0 from axiom 3 gives 0=cβ
0. And c(βd)=β(cd) for all c,dβF: by axioms 9 and 3 and the identity just proved, cd+c(βd)=c(d+(βd))=cβ
0=0, so c(βd) is an additive inverse of cd.
Claim 1. By axiom 6, 1ξ =0. Let t=β£1β£ be the absolute value of 1. Claim 1 of Properties of the Absolute Value in an Ordered Field gives 0β€t, and tξ =0 because that claim yields t=0 only for 1=0. Claim 4 of the same lemma with x=y=1, together with 1β
1=1 from axiom 6, gives t=β£1β
1β£=β£1β£β£1β£=tt. Multiplying by the inverse tβ1 of axiom 7 and using axioms 5 and 6,
1=ttβ1=(tt)tβ1=t(ttβ1)=tβ
1=t.
Hence β£1β£=1 and 0β€1.
Claim 2. From 0β€b and order axiom 1 with c=a we get 0+aβ€b+a. By axioms 2 and 4, 0+a=a and b+a=a+b, so aβ€a+b; transitivity with 0β€a gives 0β€a+b.
Claim 3. Suppose xβ€y. Order axiom 1 with c=βx gives x+(βx)β€y+(βx), that is, 0β€yβx by axiom 3. Conversely suppose 0β€yβx. Order axiom 1 with c=x gives 0+xβ€(y+(βx))+x; the left-hand side is x by axioms 2 and 4, and the right-hand side is y+((βx)+x)=y+0=y by axioms 1, 2, 3 and 4. Hence xβ€y.
Claim 4. By axiom 7 there is aβ1 with aaβ1=1, and aβ1ξ =0, since aβ1=0 would give 1=aβ
0=0 by the recorded identity, contradicting axiom 6.
Suppose 0β€aβ1 fails. As the order is total, aβ1β€0, so claim 3 applied with x=aβ1 and y=0 gives 0β€0βaβ1, and 0βaβ1=βaβ1 by axioms 2 and 4. Order axiom 2 applied to 0β€a and 0β€βaβ1 gives
0β€a(βaβ1)=β(aaβ1)=β1,
using the recorded identity. By claim 3 with x=1 and y=0, this says 1β€0; with claim 1 and antisymmetry we get 1=0, contradicting axiom 6. Hence 0β€aβ1.
Claim 5. By claim 3, 0β€yβx. Order axiom 2 applied to 0β€a and 0β€yβx gives 0β€a(yβx), and by axiom 9 and the recorded identity a(yβx)=ay+a(βx)=ay+(β(ax))=ayβax. Claim 3 applied with x replaced by ax and y by ay now gives axβ€ay.