“…Known experimental splittings for hydrogen atom tunneling span a range of more than eight orders of magnitudes, with most of them being (far) smaller than 1 cm ( 0.01 kJ mol ) [ 15 ]. For this reason, localization is the typical, but not the strict, outcome from symmetry breaking by chemical [ 3 , 16 , 17 , 18 , 19 ] or isotopic [ 4 , 5 , 20 , 21 , 22 , 23 , 24 , 25 , 26 , 27 , 28 ] substitution, internal rotation of molecular groups [ 6 , 16 , 20 , 24 , 29 ], or from environmental influences such as solvation [ 16 , 30 ], matrix embedding [ 3 , 31 , 32 ] or crystallization [ 33 ]. However, delocalization can still be observed upon excitation if either the barrier [ 3 , 5 , 21 , 25 , 26 , 29 ] or the energetic asymmetry [ 22 , 34 ] are sufficiently lowered.…”