I have essentially no experience of quantum field theory, other than a superficial knowledge of some basic ideas - my apologies if I've phrased anything unusually or made any mistakes in my question here.
For context, I've been looking at matrix methods in quantum mechanics, and I'm trying to understand a paper on a matrix model for $\Delta\to N\pi$ decay that uses chiral effective field theory to construct the Hamiltonian: https://arxiv.org/abs/1303.4157
In the paper, the bare mass $\Delta_0$ of the $\Delta$ is adjusted to account for the $\Delta\to N\pi$ interaction. This is done by: $$\Delta_0=E_\text{res}-\Sigma_{\Delta N}(k_\text{res})$$ where $E_\text{res}$ is the phenomenological value of the $\Delta$ resonance, $k_\text{res}$ is the corresponding pion momentum $E_\text{res}=\sqrt{k_\text{res}^2+m_\pi^2}$, and $\Sigma_{\Delta N}$ is given by the integral: $$\Sigma_{\Delta N}(k)=\int_0^\infty dk'\frac{k'^2g_{\Delta N}^2(k')}{\omega_\pi(k')\left[\omega_\pi(k)-\omega_\pi(k')-i\epsilon\right]}$$ where $\omega_\pi(k)=\sqrt{k^2+m_\pi^2}$ is the pion energy and $g_{\Delta N}^2$ is the $\Delta- N\pi$ coupling (which I understand to be a sort of potential energy). It is said to be related to this diagram: My question is essentially: how does one construct these integrals from these diagrams? For example, I am in particular interested in how to construct the integral for the self-energy associated with $\Delta\to\Delta \pi$ interaction, with the diagram: