Fig. 4

TTNS simulation of singlet fission in DP-Mes and structural experimental comparison. a Schematic of TTNS. The electronic system is coupled to 252 vibrational modes (ω) in DP-Mes. By means of entanglement renormalisation, a tree of linearly connected vibrational modes connected to the electronic system via entanglement renormalisation nodes (blue) can be created, allowing facile computation of non-Born-Oppenheimer dynamics for large molecules (>100 atoms, further details in Methods). The vibrational modes are grouped by symmetry and colour coded to indicate tuning (orange) or coupling (green) mode behaviour. b Projected total time-dependent mode displacements for all symmetry groups and their corresponding assignment. We remark the ~200-fold lower displacement amplitude for A2, B1 and B2 modes compared with the A1 modes. c S1 → 1TT coherence transfer Raman spectrum (blue) and resonance Raman representation of the calculated spectrum (orange). d Intrinsic 1TT Raman spectrum (purple) compared with the resonance Raman representation of calculations initiated in 1TT (orange). Calculated modes marked with an asterisk in (c) and (d) are not detected in the experimental spectrum, likely due to resonance Raman enhancement effects