“…Example 1 The schematic saturation of Ax(LLI) ∪ G + 0 consists of Ax(LLI), G + 0 and the following schematic literals: Example 2 Let RII be the theory of records of length 3 with increment whose signature is Σ RII = 3 i=1 {rstore i : rec × int → rec, rselect i : rec → int, incr : rec → rec, s : int → int} and whose set of axioms Ax(RII) consists of 3 i {rselect i (rstore i (X, Y )) = Y, rselect i (incr(X)) = s(rselect i (X))} and {rselect i ( rstore j (X, Y )) = rselect i (X)} for all i, j ∈ {1, 2, 3}, i = j. The schematic saturation of Ax(RII) ∪ G + 0 consists of Ax(RII), G + 0 and the following schematic literals, for all i ∈ {1, 2, 3}: In [18], Lemma 1 has been lifted to the case of Integer Offsets: a specific condition on the form of the schematic saturation computed by SUPC I is sufficient to show that a theory can be combined by using UPC I , along the lines of [19]. This condition is indeed satisfied for both theories LLI and RII as shown in [18], which in particular means that UPC I is also a satisfiability procedure for LLI ∪ RII.…”