A thermodynamic criterion is proposed for a generalized symmetry opera
tion in condensed matter to be well defined. It is basically the requi
rement that the spontaneous break of the defined symmetry should imply
a phase transition. This criterion is applied to the rotational symme
try in the diffraction diagram of a quasi-periodic system, showing tha
t the algebraic structure of the superspace groups is directly derivab
le from this physical requirement. Superspace symmetry, as usually def
ined in quasi-periodic systems, is the only structural geometrical pro
perty yielding rotational diffraction symmetry that is ''stable'' in t
he sense that it can only be broken if a phase transition takes place.
In contrast, some geometrical configurations producing rotational dif
fraction invariances and known as diffraction enhancement of symmetry,
, do not fulfil this stability criterion and are expected to happen on
ly fortuitously. A physical necessary condition for any generalized sy
mmetry in a condensed system is finally conjectured.