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note
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Note that the hard constraints imposed by Model II at r = σh and r = ζσ, necessary for the MC simulations, were actually never approached in the MD simulations. A routine was implemented in the MD code in order to check for this point at each time step. Thus, in practice, only the finite continuous range of the potentials of Model II was explored in the MD simulations, allowing for standard integration of the equations of motion
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