\psi \nonumber \\
&& + \frac{i \lambda^{2}K^{m}_{\
a}K^{*na}}{36\pi^{2}\varepsilon} \int {\mbox{d}}^4 x\hspace{1mm}
F^*\partial_{m}\partial_{n} F \label{2pointB}\\ 
&& +\frac{i m^{2}\lambda^{2}K^{m}_{\
a}K^{*na}}{6\pi^{2}\varepsilon} 
\int {\mbox{d}}^4 x {\mbox{d}}^4 y\hspace{1mm}
\partial_{m}\partial_{n}F(x) \square^{-1}_{x}\delta(x-y)
F^*(y). \nonumber\end{aligned}$$ Finally, adding (\[2pointA\]) and (\[2pointB\]) we obtain the divergent part of the two-point function $$\begin{aligned}
\Gamma^{(2)}_{1}\bigg|_{d.p.}&=& 
 -\frac{m^2 \lambda^2 K^{m}_{\ a}K^{*na}}{24\pi^2 \varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm} (\partial_{m}A \partial_{n}A 
+ \partial_{m}A^* \partial_{n}A^*) \nonumber \\
&& -\frac{m^2 \lambda^2
K^{mn}K_{mn}}{16\pi^2\varepsilon}\int {\mbox{d}}^4 x\hspace{1mm}
 F^2 \nonumber\\ 
&& -\frac{m^2 \lambda^2
K^{*mn}K^{*}_{mn}}{16\pi^2\varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm} F^{*2} \nonumber\\
&& +\frac{\lambda^{2}}{4\pi^{2}\varepsilon}
\int {\mbox{d}}^8 z\hspace{1mm} \Phi^{+}\Phi \nonumber\\
&& - \frac{\lambda^{2}K^{m}_{\ a}K^{*na}}{6\pi^{2}\varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm} A^*\bigg(m^{2}
+ \frac{\square}{6}\bigg)\partial_{m}\partial_{n} A \nonumber\\
&& + \frac{i\lambda^2 K^{m}_{\ a}K^{*n}_{\ b}}{24\pi^{2}\varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm} \bar{\psi}(\bar{\sigma}^{b}\partial^{a}
-\bar{\sigma}^{a}\partial^{b}+ i\varepsilon^{abcd}\bar{\sigma}_{d}
\partial_{c})\partial_{m}\partial_{n} \psi \nonumber \\
&& - \frac{i\lambda^2 K^{m}_{\ a}K^{*na}}{12\pi^{2}\varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm}
\bar{\psi}\bar{\sigma}_{n}
\partial_{m}\bigg(m^{2}-\frac{\square}{6}\bigg)\psi \nonumber \\
&& + \frac{i\lambda^2 K^{m}_{\ a}K^{*na}}{72\pi^{2}\varepsilon} 
\int {\mbox{d}}^4 x\hspace{1mm}
\bar{\psi}\bar{\sigma}^{l}\partial_{l}\partial_{m}\partial_{n} \psi 
\nonumber \\
&& + \frac{\lambda^{2}K^{m}_{\ a}K^{*na}}{72\pi^{2}\varepsilon}
\int {\mbox{d}}^4 x\hspace{1mm}
F^*\partial_{m}\partial_{n} F \nonumber\\ 
&& + \frac{m^{2}\lambda^{2}K^{m}_{\ a}K^{*na}}{12\pi^{2}\varepsilon}
\int {\mbox{d}}^4 x {\mbox{d}}^4 y\hspace{1mm}
\partial_{m}\partial_{n}F(x) \square^{-1}_{x}\delta(x-y)
F^*(y). \label{2pointAll}\end{aligned}$$ We immediately see that the divergences appearing in (\[2pointAll\]) cannot be absorbed by counterterms since the terms appearing in (\[2pointAll\]) do not exist in the classical action. All terms in (\[2pointAll\]) quadratic in the deformation parameter are also quadratic in fields. However, the 