Minimal-subtraction two-point counterterms in cubic scalar theory ($\delta Z=-g^2/[6(4\pi {)}^3ϵ],\delta m^2=-g^2{m}^2/[(4\pi {)}^3ϵ]$)

With additive counterterms $\frac{1}{2}\delta Z(\partial \varphi {)}^2+\frac{1}{2}\delta m^2{\varphi }^2$, their Euclidean propagator insertion is $-(\delta Z{k}^2+\delta m^2)$. These minimal subtraction scheme coefficients cancel the cubic bubble insertion. A bare mass shift also subtracts $m^2\delta Z$ after wavefunction renormalization; it is not the same coefficient as the additive mass counterterm.