For a connected Feynman diagram with external valence n and cubic, quartic and sextic vertices, counting half-edges gives 2I+n=3V3+4V4+6V6. Using L=I−(V3+V4+V6)+1 yields L−1+n/2=V3/2+V4+2V6. Since each summand lies between half and twice its vertex count, the displayed bounds follow. More generally vertices of valence between rmin and rmax give (rmin/2−1)V≤L−1+n/2≤(rmax/2−1)V.