By recasting the Klein–Gordon equation as an eigen-equation in the coupling parameter v>0,v>0, the basic Klein–Gordon comparison theorem may be written f1≤f2⇒G1(E)≤G2(E)f1≤f2⇒G1(E)≤G2(E), where f1f1 and f2f2 are the monotone nondecreasing shapes of two central potentials V1(r)=v1f1(r) and V2(r)=v2f2(r) on [0,∞). Meanwhile, v1=G1(E) and v2=G2(E) are the corresponding coupling parameters that are functions of the energy E∈(−m,m). We weaken the sufficient condition for the ground-state spectral ordering by proving (for example in d=1 dimension) that if ∫x0[f2(t)−f1(t)]φi(t)dt≥0, the couplings remain ordered v1≤v2, where i=1 or 2, and {φ1,φ2} are the ground-states corresponding, respectively to the couplings {v1,v2} for a given E∈(−m,m).. This result is extended to spherically symmetric radial potentials in d>1 dimensions.