“…[1][2][3][4][5][6] In MCTDH, the time-dependent Schrödinger equation (TDSE) is solved by introducing a wavefunction ansatz comprising a sum of Hartree products of single-particle functions (SPFs), along with their complex expansion coefficients; using the Dirac-Frenkel time-dependent variational principle, [7][8][9] one can then derive equations-of-motion for both the expansion coefficients and the SPFs, leading to an efficient method for propagating wavepackets which can, in principle, be converged to the exact quantum-mechanical result. The range of systems modelled to date with MCTDH is continually growing, spanning non-adiabatic dynamics in organic molecules, 2,10,11 transport on model surfaces, [12][13][14] and organometallic complexes. 15,16 In practice, two important general factors have constrained the application domain of MCTDH simulations.…”