renormalized. The calculations are based on the TRV $NN$ potential derived in the previous section (and summarized in Appendix \[app:pot\]) and on the (strong interaction) PC $NN$ potential obtained by Entem and Machleidt at next-to-next-to-next-to-next-to-leading order (N4LO) [@DR15]. These potentials are regularized with a cutoff function depending on a parameter $\Lambda$; its functional form, however, is different from the adopted here for $V_{TRV}$. Below we consider the versions with $\Lambda=450$ MeV, $500$ MeV, and $550$ MeV. The calculations of $\tri$ and $\hel$ EDMs also include the $NNN$ TRV nuclear potential derived in Sec. \[sec:NNNtrv\] and the PC $NNN$ potential derived in $\chi$EFT at N2LO. As for the $NN$ PC potential, it depends on a cutoff parameter $\Lambda$ which is chosen to be consistent with those in the PC and TRV $NN$ potentials. The three-nucleon PC potential depends, in addition, on two unknown LECs, denoted as $c_D$ and $c_E$ and also on the LECs $c_1$, $c_3$ and $c_4$. In this work, we use the values reported in Table III of Ref. [@LE18]. The ${V_{TRV}}^{(3\pi,1)}$ term of the TRV potential depends on the LECs $c_1$, $c_2$ and $c_3$ which are taken from Table II of Ref. [@DR15] and summarized here in Table 