Each result cited is universally quantified over the data in its own statement. The sum y+h and the difference yβx of points of Rn are formed coordinatewise, by Sum of Points of Rn and Difference, Dot Product, and Orthogonality in Rn, and two points of Rn are equal exactly when their coordinates agree, by claim 1 of Euclidean Points as Tuples of Real Numbers; hence identities such as (y+m)βx=(yβx)+m, (yβx)+x=y and (z+x)βx=z, and the cancellation y+a=q+aβy=q, hold in Rn because they hold coordinatewise in the field R. For AβRn and hβRn write A+h={z+h:zβA}, as in Translation and Reflection Invariance of Lebesgue Measure on ββΏ; 1Aβv denotes the pointwise product of the indicator with a map v.
Periodicity of wxβ. Let yβRn and mβZn. Then (y+m)βx=(yβx)+m, so wxβ(y+m)=w((yβx)+m)=w(yβx)=wxβ(y) by the periodicity of w.
Measurability of wxβ. Let B be a Borel subset of R. Then wβ1(B)βB(Rn) since w is measurable, and
wxβ1β(B)={yβRn:yβxβwβ1(B)}=wβ1(B)+x,
because yβxβwβ1(B) holds exactly when y=z+x for some zβwβ1(B), namely z=yβx. The set wβ1(B)+x is Borel by claim 1 of Translation and Reflection Invariance of Lebesgue Measure on ββΏ. Hence wxβ is measurable by Measurable Map, and the Set of Measurable Maps.
Integrability and the integral. Let a=βx be the additive inverse of x, the point with coordinates βxiβ by claim 2 of Euclidean Space Rn is a Real Vector Space, so that y+a=yβx for every yβRn by claim 3 of that proposition. By The Half-Open Unit Cell Tiles Euclidean Space (v), applied to w and h=a, the map 1Q+aβw is integrable and
β«Rnβ1Q+aβwdΞ»nβ=β«Rnβ1QβwdΞ»nβ.
Let f=1Q+aβw, which is measurable, since Integrable Functions and Their Lebesgue Integral defines integrability only for measurable maps. For yβRn one has f(y+a)=1Q+aβ(y+a)w(y+a)=1Qβ(y)wxβ(y): indeed y+a=yβx, and y+aβQ+a holds exactly when y+a=q+a for some qβQ, that is, by cancellation, exactly when yβQ. So the map yβ¦f(y+a) is 1Qβwxβ. By claim 3 of Translation and Reflection Invariance of Lebesgue Measure on ββΏ, applied to f and a, the map yβ¦f(y+a) is integrable, since f is, and
β«Rnβ1QβwxβdΞ»nβ=β«Rnβf(y+a)dΞ»nβ(y)=β«RnβfdΞ»nβ=β«Rnβ1QβwdΞ»nβ.