“…With a full Fokker‐Planck code, one can solve today simultaneously the following processes: radial diffusion, pitch angle diffusion, energy diffusion, cross energy and pitch angle diffusion, Coulomb collision, and anomalous diffusion. Among the most well‐established Fokker‐Planck codes are the ONERA Salammbô code (e.g., Beutier & Boscher, ; Bourdarie et al, , , ; Pugacheva et al, ; Beutier et al, 2005; Varotsou et al, , ; Maget et al, ; Herrera et al, ), the British Antarctic Survey (BAS) Radiation Belt Code (e.g., Glauert et al, , ; Glauert & Horne, ; Horne et al, ; Meredith et al, , ), the VERB 3‐D code (e.g., Subbotin & Shprits, ; Shprits et al, ; Subbotin et al, , ; Kim et al, 2011, Kim et al, ; Drozdov et al, ) recently extended to a 4‐D version (e.g., Aseev et al, ; Shprits et al, ) to soon incorporate models of nonlinear wave‐particle interactions, the University of California, Los Angeles (UCLA) 3‐D diffusion code (e.g., Tao et al, ; Li et al, ; Li, Ma, et al, ; Ma et al, , , , Ma et al, that incorporates the (UCLA) Full Diffusion Code (e.g., Ni et al, 2008, Ni et al, ; Shprits & Ni, 2009) in order to compute diffusion coefficients (similarly to VERB 3‐D/4‐D), the radiation belt code of the Space Vehicles Directorate of the U.S. Air Force Research Laboratory (AFRL) (e.g., Albert, , ; Albert et al, ; Albert & Young, ; Selesnick, Albert, & Starks, ), the LANL Dynamic Radiation Environment Assimilation Model (DREAM) 1‐D (e.g., Tu et al, 2009; Reeves et al, ; Welling et al, ) and 3‐D codes (Camporeale et al, , ; Cunningham, ; Cunningham et al, ; Tu et al, ), the Commissariat à l'Energie Atomique (CEA) CEVA code (Réveillé, ; Ripoll & Mourenas, 2012; Ripoll, Chen, et al, , Ripoll, Reeves, et al, , Ripoll et al, , ), and the STEERB code developed in China (e.g., Su et al, …”