Note that the number of elements of
and
is
. The notion of symmetry we propose here takes into account all the “reoccurring” subsets, where the transformation relating both has to belong to the prescribed group. The last requirement just ensures that only one of the pairs
and
is counted among these symmetries.
The following statement certainly expresses what one would expect. We will nevertheless include the argument, mainly to introduce a useful parametrization of melodies.
Proof: Let
be a melody,
, and set
,
,
. By definition, all the differences
have positive first component. The main observation for what follows is that a symmetry
-pair in
with respect to
is nothing but a pair of pairs
of tones in
,
less than or equal to
, such that
, i.e.
. Setting
,
, the 1-symmetry
can be expressed in the form of the equation
Noting that a symmetry
-pair,
, can be thought of as a specific combination of 1-symmetries, it is thus described by finitely many linear relations of the above type. In other words, for a melody
to display a symmetry
-pair means for the corresponding point
in
(more precisely, in the
-fold product of the right half-plane in
) to lie in the intersection of the hyperplanes described by the linear relations above. This geometric statement expresses the claim of the proposition in a more precise way.
Remark 1 One can compute the number of possible linear relations. Using, in addition, (musically realistic) bounds for the onsets and pitches of a melody, this, together with the fact that tones are supposed to have integer components, may be used to obtain a more precise than just the genericity formulation of the proposition. Moreover, including pitch inversion and retrograde leads to more linear relations and hence does not alter the statement.