Exponents of 0.71 and 0.75 were reported for model PDMS networks made of strands below the entanglement molecular weight or an exponent of 0.4 for gelatin gels. For the data of Gnanou et al. excluding the networks with a sol fraction beyond 10 %, see table and 31 in Ref. , one obtains exponents of 0.52 and 0.92 for the short and the long polymers, respectively. A simulation study reported exponents increasing from 0.25 to 0.55 with increasing length of still quite short chains. In contrast to this, we found only a very weak increase of the exponent for increasing 𝑁. Altogether, the dependence on 𝜙 0 has not been settled yet, but this open question could be advanced by using network architectures as ours that are less susceptible to network defects.