Let us now consider the set
of all the squared terms sequences
associated to a sequence
.
From Eq. 5, we have
and therefore
is a subset of the vector space
generated by the geometric sequences
,
and
.
This 3-dimension vector space is the set of the sequences verifying
the recurrence relation of third order whose characteristic polynomial
is
namely
| Sequence | U | V | W |
When recurrence Eq. 4 is really a recurrence of
second order (i.e.
and
),
the vector space
is spanned by
,
,
if and only
if vector space
is spanned by
.
Let us now consider the even and odd subsequences
and
defined by
and
.
In the general case, their generating functions can be obtained by
Let
be a non-geometric
sequence verifying a linear recurrence of second order. Let
be the roots of the characteristic polynomial. Then for all
:
In the genuine Fibonacci case, this result is the formerly stated relation Eq. 2.
In order to see if other relations of this kind can be found, we have
to understand why relation Eq. 17 holds. On the
left side, we have a linear combination of squared terms. The poles
involved in the corresponding generating function are
.
On the right side, we have a combination of terms coming from "arithmetic
subsequences", i.e.
. But, from Eq. 5,
we have :
For fixed
, all the arithmetic subsequences
obey to the same linear recurrence of order 2, whose poles are
and
.
The only way to have the same poles on both sides is to use only
(the odd and even sub-series) on the right, and to avoid the
pole on the left. Therefore this left side must embed an action that
results in the apparition of the factor
in the generating function. But this factor codes for the action
acting over sequences: the left member is necessarily a linear combination
of the sequences obtained by shifting the sequence
.
Applied to the (genuine) Fibonacci sequence, this proves that the
only combination of squares that can be linearized are those build
upon
by shifts and linear combinations. For
example, the expression
, whose
generating function is