Spectroscopic factors, extracted from one-neutron knockout and Coulomb dissociation reactions, for transitions from the ground state of 33 Mg to the ground-state rotational band in 32 Mg, and from 32 Mg to low-lying negative parity states in 31 Mg, are interpreted within the rotational model. Associating the ground state of 33 Mg and the negative parity states in 31 Mg with the 3 2 [321] Nilsson level, the strong coupling limit gives simple expressions that relate the amplitudes (C j ) of this wavefunction with the measured cross-sections and derived spectroscopic factors (S j ). To obtain a consistent agreement with the data within this framework, we find that one requires a modified 3 2 [321] wavefunction with an increased contribution from the spherical 2p 3/2 orbit as compared to a standard Nilsson calculation. This is consistent with the findings of large scale Shell Model calculations and can be traced to weak binding effects that lower the energy of low-orbitals.