Journal of Luminescence 22 (1981) 273—284 273
North-Holland Publishing Company
RADIATIVE ENERGY TRANSFER
I. GENERAL EQUATIONS
J.C. CONTE and J.M.G. MARTINHO
Centro de Quirnica Fisica Molecular, Complexo I, Inst ituto Superior Técnico, 1000 Lisboa,
Portugal
Received 11 April 1980
Revised manuscript received 29 September 1980
A set of equations is derived which makes possible to study the radiative energy transfer
process whereby the photons emitted by the energy donor are absorbed by the energy
acceptor and so increase the efficiency of the overall energy transfer. It is shown that the
coefficients describing the radiative transfer which appear in the expressions for the
intensities of the energy donor and the energy acceptor are not the same, due to the fact
that past of the fluorescence absorbed by the acceptor comes from radiation which is not
detected as donor emission when there is no acceptor present. The general equations
derived are applied to two particular cases commonly considered: measurements in reflec-
tion, where the fluorescence emission is observed from the same face of the absorption and
measurements in transmission where the fluorescence emission is observed from the
opposite face of the cell.
1. Introduction
It is well known [1,2] that in a binary liquid system containing two
fluorescent molecules Y and Z it is possible to observe fluorescent emission
from both species when the solution is excited with uv radiation of adequate
energy, even when the optical density for absorption by one of the species is so
low that it is valid to assume that all the excitation is absorbed by the other.
This effect shows that an energy transfer process between an energy donor
(which absorbs almost all the energy of excitation) and an energy acceptor is
taking place.
This energy transfer process may be either radiative if photons are emitted
by the energy donor and subsequently absorbed by the acceptor or nonradia-
tive if it takes place without any emission followed by absorption.
That both processes may take place is widely accepted. The fact that
radiative transfer is mainly important for solutions where the concentration of
the energy acceptor is low and the quantum yield of the energy donor is high
[3] has been used by several authors to choose the systems under study such as
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