In every investigation of a real physical system one is always
forced to simplify and idealise the true properties of the system. This
process of idealisation of the problem can never be avoided and constitutes
the real essence of the physical transaction of a real problem.
In fact, in order to construct a mathematical model of the system under
observation, one have to choose the basic factors governing just those
features of the behaviour of the system which are of his interest neglecting
all the others.
An attempt of trick this procedure by now consolidated from the different
centuries of the physical experience doesn't bring in general that to a
featureless bulk of information that should be treated by means of the
mathematical formalisms whose solution would be extremely cumberstone,
if not altogether impossible.
On the other side often the schematization of a simple real system allows
to obtain of the useful models to explain the behaviour of more complex
systems.
An important aspect to hold in account is that the nature of the idealisation
permissible in the analysis of a problem is determined by the whole problem
and therefore depends not only on the properties of the analysed system
but also from the questions which we will to answer with our analysis.
Since an idealisation of the problem is in any case inevitable the question
arise of how far is possible to idealise the properties of the system still
obtaining good results.
Only experiments are able to give an answer to this question and to
legitimate the idealisation of the real system.
The idealisation of the problem seem to be particularly difficult to
make in the case of the study, by means of physical formalisms, of the
biological systems and this difficulty is not probably extraneous to the
scrubby growth of the biophysics that often appear as a mere application
of physical measurement techniques to the biological systems.
In this paper we will expose some characteristic of a biophysical phenomenon
which seems to be particularly proper for begin an analysis of the biological
systems departing from a physical point of view.
In 1950 B Strehler observed a totally unaspected light emission from
green plants some seconds after illumination that at the moment was interpreted
as energy remitted from the pigment systems associated to PSII
Starting from 1980 some papers appeared in literature [1,2,3]
demonstrating that this light emission was more general and that also cell
cultures without any photosystem after illumination exhibit a relaxation
dynamics approximated by a hyperbolic decay law .
In the last few years a lots of experimental works [4,13]
on several biological systems have shown that there is a close connection
between the biological state of the system and the parameters of this phenomenon,
referred in literature as delayed fluorescence, delayed luminescence (D.L.),
delayed light emission or induced photon emission.
The study of this phenomenon seems to be particularly proper for begin
an analysis of the biological systems departing from a physical point of
view.
D.L. is in fact a phenomenon relatively simple to measure but able to
furnish, by means of a measure of the electromagnetic fields received and
emitted by the biological system, important information on the fields and
the structures inside to the same system.