“…these include µ = δ 1 −δ 2 , the difference of two Dirac measures, where F (s) := Lµ(s) = e −s − e −2s and F (−sA) = T (t) − T (2t). More importantly, the theorem applies to many other examples, such as dµ(t) = (χ [1,2] − χ [2,3] )(t)dt and µ = δ 1 − 3δ 2 + δ 3 + δ 4 , which are not accessible with the methods of [1,9,10,14].…”