QCD Laplace sum-rules must satisfy a fundamental (Holder) inequality if the
y are to consistently represent an integrated hadronic cross-section. After
subtraction of the pion-pole, the Laplace sum-rule of pion currents is sho
wn to violate this fundamental inequality unless the u and d quark masses (
respectively denoted by m(u) and m(d)) are sufficiently large, placing a lo
wer bound on the 1 eV <(MS)over bar> running masses. (C) 1999 Elsevier Scie
nce B.V. All rights reserved.