All-order spurion-corrected superpropagators and superfield Feynman rules are employed to sys- In the case of supersymmetric theories, the effective potential can be directly calculated in superspace, by using supergraphs. In general, the supereffective action is described by two functions of the chiral and the antichiral superfields; one is required to be a holomorphic function and the other one, called Kähler potential, less constrained, is required to be just a real function. The holomorphic part of the superpontential is very constrained, which is reflected in various nonrenormalization theorems, leading to results to all orders in perturbation theory [1], and even nonperturbative results in some cases [2]. For models with spontaneous supersymmetry (SUSY) breaking, the effective potential can be calculated by using superspace techniques even if soft explicit breaking terms are introduced in the superspace action; this yields spurion insertions. These terms have been carefully classified and studied by Girardello and Grisaru [3]. This approach to study SUSY breaking is very powerful because it leaves most of the supersymmetric structure intact. In fact, as the full supersymmetric and the supersymmetry breaking terms are represented as interactions in superspace, the renormalization can be performed systematically directly in superspace.In general, the background field method is adopted to calculate the effective potential.In this method, the scalar fields of the theory are each separated into a constant classical background plus quantum fluctuations. Using this approach, the effective potential is equal