Use the reverse absorption order on the incline:
This is exactly the relation given by the pairs . Indeed, if and , then by additive idempotence, associativity and commutativity. Conversely expresses as , so is one of these pairs.
Additive idempotence gives , hence reflexivity. If and , then
so the relation is transitive. In fact it is antisymmetric as well: and , together with commutativity, imply . Thus the relation is a partial order, and therefore a quasi-order. It is the reverse of the usual join order of an incline; keeping this reversal is essential for the well-quasi-ordering conclusion.
Both operations are order-preserving for this order. If , then by additive idempotence, while distributivity gives . The multiplicative absorption identity also says
Thus multiplying a monomial by another factor moves upward in the reverse absorption order.
Suppose the incline is generated by . Repeated distributivity, followed by commutativity and additive idempotence, expresses every element as a finite nonempty sum
No multiplicative identity is assumed: a zero exponent means that the corresponding generator is omitted, and every displayed monomial has at least one factor. Different supports may represent the same element; uniqueness is unnecessary.
Associate to its upward-closed exponent set
If , each monomial of is either equal to, or a multiplicative extension of, a monomial of . It is absorbed by that earlier monomial, and hence by the full sum . Adding the terms of one at a time gives
For equal exponent vectors the first absorption is additive idempotence; for strictly larger vectors it is the incline's multiplicative absorption. Thus the issue is to prove that exponent upsets are well-quasi-ordered by reverse inclusion, not merely to apply Dickson's lemma to individual exponents.
We prove the reverse-inclusion well-quasi-ordering of monomial ideals, equivalently of all upward-closed subsets of , by induction on . For the sets are tails and the empty set; reverse inclusion orders their endpoints as , a well-order. The case , if needed for the induction, is just a finite family.
For an upset , let . These are upsets of and satisfy . They stabilize. Indeed the union has a finite minimal basis by Dickson's lemma: an infinite set of minimal elements would be an antichain in the componentwise well-quasi-ordering of . Each basis element appears in some slice, and after the largest of these finitely many indices the slice contains the entire upset .
Choose a stabilization index , and encode by the finite word and the final slice . The induction hypothesis makes slices a well-quasi-ordering by reverse inclusion. Higman's lemma, proved in Question 3 below, makes their finite words a well-quasi-ordering; finite product closure of well-quasi-orderings also compares the final slices. Thus in every infinite sequence of upsets there are earlier and later with a strictly increasing matching of the earlier pre-stabilization slices into the later ones, such that
Since and the -slices increase, for . For , . Therefore , completing the induction.
Now choose one finite support for each term of an arbitrary infinite sequence in the finitely generated incline. The result supplies with , and the preceding absorption calculation gives . Hence every finitely generated incline is well-quasi-ordered by the specified reverse absorption order. The proof allows all additional algebraic identifications among the generators.

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