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The monotonic Quartic Spline Method (QSM) for conservative transport problems., , and . J. Comput. Phys., 229 (4): 1150-1166 (2010)The Met Office Unified Model Global Atmosphere 6.0/6.1 and JULES Global Land 6.0/6.1 configurations, , , , , , , , , and 28 other author(s). Geoscientific Model Development, 10 (4): 1487--1520 (Apr 11, 2017)Aspects of the dynamical core of a nonhydrostatic, deep-atmosphere, unified weather and climate-prediction model., and . J. Comput. Phys., 227 (7): 3445-3464 (2008)An inherently mass-conserving semi-implicit semi-Lagrangian discretization of the deep-atmosphere global non-hydrostatic equations, , , , , , , , , and 1 other author(s). Q.J.R. Meteorol. Soc., 140 (682): 1505--1520 (Jul 1, 2014)The UM, a fully-compressible, non-hydrostatic, deep atmosphere GCM, applied to hot Jupiters, , , , , , , , and . (Nov 8, 2013)A mixed finite-element, finite-volume, semi-implicit discretisation for atmospheric dynamics: Spherical geometry., , , , , , , , , and 4 other author(s). CoRR, (2024)Runge-Kutta IMEX schemes for the Horizontally Explicit/Vertically Implicit (HEVI) solution of wave equations., , and . J. Comput. Phys., (2013)Application of the parabolic spline method (PSM) to a multi-dimensional conservative semi-Lagrangian transport scheme (SLICE)., , and . J. Comput. Phys., 225 (1): 935-948 (2007)