The semigroup formalism permits a general description of relaxation process
es in quantum mechanical systems coupled to Markovian baths. From its defin
ition, the semigroup formalism should be expressed in terms of the dissipat
ive and relaxation coupling of the eigenstates of the quantum system to the
bath modes. Often, for convenience both in calculation and in physical int
erpretation, it is more straightforward to couple local states of the quant
um mechanical system to the bath. Within a simple two-site system, we exami
ne the generalities of these two different coupling schemes, noting situati
ons in which they are the same and situations for which substantial differe
nces occur.