Let g be the plane rotation in coordinates (i,j) with parameters (a,b), a2+b2=1. By the definition of the dot product, g(v)β
g(u) is the sum over coordinates of the products of corresponding coordinates. The coordinates with index kβ/{i,j} contribute vkβukβ, unchanged. The coordinates i and j contribute
(aviβ+bvjβ)(auiβ+bujβ)+(βbviβ+avjβ)(βbuiβ+aujβ)=(a2+b2)(viβuiβ+vjβujβ)+ab(viβujβ+vjβuiβ)βab(viβujβ+vjβuiβ)=viβuiβ+vjβujβ.
Summing all contributions gives g(v)β
g(u)=vβ
u.
For a finite composition h=gLβββ―βg1β, the identity h(v)β
h(u)=vβ
u follows by applying the single-rotation identity L times (and holds trivially for the empty composition, which is the identity map). Finally, if w1β,β¦,wpβ is an orthonormal family, then h(wiβ)β
h(wiβ)=wiββ
wiβ=1 and h(wiβ)β
h(wkβ)=wiββ
wkβ=0 for i<k, so h(w1β),β¦,h(wpβ) is an orthonormal family. β