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Combining Probabilities
Consider two distinct possible outcomes,
and
,
of an observation made on the system
, with probabilities of
occurrence
and
, respectively. Let us determine the probability of
obtaining either the outcome
or the outcome
, which we shall denote
.
From the basic definition of probability,
|
(2.2) |
where
is the number of systems in the ensemble that exhibit
either the outcome
or the outcome
. It is clear that
|
(2.3) |
if the outcomes
and
are mutually exclusive (which must be the case
if they are two distinct outcomes). Thus,
|
(2.4) |
We conclude that the probability of obtaining either the outcome
or the outcome
is the
sum
of the individual probabilities of
and
. For instance, with a six-sided die, the probability of throwing any particular number (one to six) is
, because all of the possible outcomes are considered to be equally
likely. It follows, from the previous discussion, that the probability of
throwing either a one or a two is
, which equals
.
Let us denote all of the
, say, possible outcomes of an observation
made on the system
by
, where
runs from
to
. Let us
determine the probability of obtaining
any of these outcomes. This quantity is clearly unity,
from the basic definition of probability, because every one
of the systems in the ensemble must
exhibit one of the possible outcomes. However, this quantity is also equal to
the sum of the probabilities of all the individual outcomes, by Equation (2.4),
so we conclude that
this sum is equal to unity. Thus,
|
(2.5) |
which is called the normalization condition, and must be satisfied by
any complete set of probabilities. This condition is equivalent to the
self-evident statement that an observation of a system must definitely
result in one of its possible outcomes.
There is another way in which we can combine probabilities. Suppose
that we
make an observation on a state picked at random from the ensemble, and then
pick a second state, completely independently, and
make another observation. Here, we are assuming that the first
observation does not influence the second observation in
any way. In other words, the two
observations are statistically independent.
Let us determine the probability of obtaining
the outcome
in the first state and
the outcome
in the second state, which we shall denote
.
In order to determine this probability, we have to form an ensemble of all
of the possible pairs of states that we could choose from the ensemble,
. Let us denote this ensemble
.
It is obvious that the number of pairs of states in this new
ensemble is just the
square of the number of states in the original ensemble, so
|
(2.6) |
It is also fairly obvious that the number of pairs of states
in the ensemble
that exhibit the
outcome
in the first state, and
in the second state,
is just the
product of the number of states that exhibit the outcome
,
and the number of states that exhibit the outcome
, in the original
ensemble.
Hence,
|
(2.7) |
It follows from the basic definition of probability that
|
(2.8) |
Thus, the probability of obtaining the outcomes
and
in two statistically independent
observations is the product of the individual probabilities of
and
. For instance, the probability of throwing a one and then a two
on a six-sided die is
, which equals
.
Next: Two-State System
Up: Probability Theory
Previous: What is Probability?
Richard Fitzpatrick
2016-01-25