FRET occurs through dipole-dipole coupling between the excited-state donor and ground-state acceptor chromophores. When the donor absorbs a photon and reaches its excited state, this energy can transfer to a nearby acceptor without photon emission–provided the acceptor's absorption spectrum overlaps the donor's emission spectrum.
The efficiency of this transfer depends critically on distance, orientation, and spectral overlap. At the Forster radiusLoading... (R0), transfer efficiency is exactly 50%. At distances much shorter than R0, transfer approaches 100%; at distances greater than 2×R0, it becomes negligible.
This steep distance dependence–following an inverse sixth-power relationship–transforms FRET into a molecular ruler capable of distinguishing proteins in genuine contact from those merely colocalized in the same cellular region.