Additive Haar measures on Euclidean space and Lebesgue measure on ι → ℝ #
Every additive Haar measure μ on EuclideanSpace ℝ ι is a positive finite multiple a • volume
of the volume measure, and ofLp carries the volume measure to Lebesgue measure on ι → ℝ. So
ofLp carries μ to a • volume, and μ gives the preimage under ofLp of a set S ⊆ ι → ℝ
the measure a * volume S. In particular a cube, the preimage of a sup-norm closed ball, can be
compared with the concentric Euclidean ball: the cube of half-side r has measure at most √nⁿ
times that of the Euclidean ball of radius r, since that ball contains the cube of half-side
r / √n.
Main results #
EuclideanSpace.exists_map_toLp_symm_eq_smul: an additive Haar measure is carried byofLpto a positive finite multiple of Lebesgue measure.EuclideanSpace.measure_preimage_ofLp: the measure of a preimage underofLp.EuclideanSpace.measure_preimage_ofLp_closedBall,EuclideanSpace.measure_preimage_ofLp_ball: the measure of a cube.EuclideanSpace.measure_preimage_ofLp_closedBall_le: a cube has measure at most√nⁿtimes that of the Euclidean ball of the same radius.EuclideanSpace.measurePreserving_consEquivL: splitting off the first coordinate identifies the volume ofℝⁿ⁺¹with the product of the volumes ofℝandℝⁿ.
An additive Haar measure on EuclideanSpace ℝ ι is carried by ofLp to a positive finite
multiple of Lebesgue measure on ι → ℝ.
If ofLp carries μ to a • volume, then μ gives the preimage of S the measure
a * volume S.
If ofLp carries μ to a • volume, then μ gives the cube of half-side r ≥ 0 the
measure a (2r)ⁿ.
If ofLp carries μ to a • volume, then μ gives the open cube of half-side r > 0 the
measure a (2r)ⁿ.
The Euclidean ball B(x, r) lies in the cube of half-side r centred at x, whose measure
is at most √nⁿ times that of the ball.
Splitting off the first coordinate carries the product of Lebesgue measure on ℝ and the volume
of ℝⁿ to the volume of ℝⁿ⁺¹.
Projection onto the unique coordinate of a Euclidean line preserves actual volume.
The unique-coordinate projection is a measurable embedding, so normalized volume transport also applies to arbitrary restricted integrals.
Integrating a function of the unique coordinate of a Euclidean line over the preimage of s
is integrating it over s.