We introduce a cluster DMFT (Dynamical Mean Field Theory) approach to study the normal state of the iron pnictides and chalcogenides. In the regime of moderate mass renormalizations, the self-energy is very local, justifying the success of single site DMFT for these materials and for other Hunds metals. We solve the corresponding impurity model with CTQMC (Continuous Time Quantum Monte-Carlo) and find that the minus sign problem is not severe in regimes of moderate mass renormalization.The unexpected discovery of superconductivity in the iron pnictide based materials has opened a new era of research in the field of condensed matter physics.[1] Multiple approaches, starting from weak coupling such as the random phase approximation (RPA) and strong coupling approaches using lessons learned from the t-J model, have been proposed, but there is not yet consensus in the community of what constitutes the proper theoretical framework for describing these systems.[2] It has been proposed that iron pnictides and chalcogenides are important not only because of their high temperature superconductivity, but because their normal state properties represent a new class of strongly correlated systems, the Hunds metals. They are distinct from doped Mott Hubbard systems, in that correlations effects in their physical properties derive from the Hunds rule coupling J, rather than the Hubbard U. [3,4] Many other interesting Hunds metals have been recognized, as for example Ruthenates [5] and numerous 3d and 4d compounds [6].Dynamical Mean Field Theory [7](DMFT) and its cluster extensions [8,9] have provided a good starting point for the description of Mott Hubbard physics. It is now established that it describes many puzzling properties of three dimensional materials such as Vanadium oxides near their finite temperature Mott transition. [10] In materials such as cuprates, as the temperature is lowered, the description in terms of single site DMFT gradually breaks down. New phenomena such as momentum space differentiation and the opening of a pseudogap takes place, and cluster DFMT is essential. How different cluster sizes and methods captures these effects has been explored intensively. [14,29,[36][37][38][39][40][41] The iron pnictides and chalcogenides have been extensively studied using LDA+DMFT by several groups. [3,4,[42][43][44] It has been argued using the GW method, that the frequency dependence of low order diagrams in perturbation theory in these materials is very local.[45] However, because of the difficulties posed by the multiorbital nature of these compounds, the accuracy of the local approximation beyond the GW level has not been examined and is the main goal of this paper.Building on the work of Ref. 46, we introduce a cluster extension for the treatment of iron pinctides, which is numerically tractable using CTQMC. By comparing single site and cluster DMFT, we establish that in a broad range of parameters where the mass renormalizations are of the order of 2 to 3, which corresponds to the experimental situation in...