), and they exhibit dihedral symmetry. The many-to-one phenomenon is known as
aliasing. An example of infinite dihedral symmetry is in
aliasing of real-valued signals. When sampling a function at frequency (intervals ), the following functions yield identical sets of samples: {{math|{sin(2(
f +
Nf)
t +
φ),
N 0, ±1, ±2, ±3, . . . }}}. Thus, the detected value of frequency is
periodic, which gives the translation element . The functions and their frequencies are said to be
aliases of each other. Noting the trigonometric identity: : \sin(2\pi (f+Nf_s)t + \varphi) = \begin{cases} +\sin(2\pi (f+Nf_s)t + \varphi), & f+Nf_s \ge 0, \\[4pt] -\sin(2\pi |f+Nf_s|t - \varphi), & f+Nf_s we can write all the alias frequencies as positive values: |f+Nf_s|. This gives the reflection () element, namely ↦ . For example, with and ,
reflects to , resulting in the two left-most black dots in the figure. The other two dots correspond to and . As the figure depicts, there are reflection symmetries, at 0.5, , 1.5, etc. Formally, the quotient under aliasing is the
orbifold [0, 0.5], with a
Z/2 action at the endpoints (the orbifold points), corresponding to reflection. ==See also==