Generalized polar coordinate change #
Consider an n-dimensional normed space E and an additive Haar measure μ on E.
Then μ.toSphere is the measure on the unit sphere
such that μ.toSphere s equals n • μ (Set.Ioo 0 1 • s).
If n ≠ 0, then μ can be represented (up to homeomorphUnitSphereProd)
as the product of μ.toSphere
and the Lebesgue measure on (0, +∞) taken with density fun r ↦ r ^ n.
One can think about this fact as a version of polar coordinate change formula for a general nontrivial normed space.
If μ is an additive Haar measure on a normed space E,
then μ.toSphere is the measure on the unit sphere in E
such that μ.toSphere s = Module.finrank ℝ E • μ (Set.Ioo (0 : ℝ) 1 • s).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The measure on (0, +∞) that has density (· ^ n) with respect to the Lebesgue measure.
Equations
- MeasureTheory.Measure.volumeIoiPow n = (MeasureTheory.Measure.comap Subtype.val MeasureTheory.volume).withDensity fun (r : ↑(Set.Ioi 0)) => ENNReal.ofReal (↑r ^ n)
Instances For
The intervals (0, k + 1) have finite measure MeasureTheory.Measure.volumeIoiPow _
and cover the whole open ray (0, +∞).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The homeomorphism homeomorphUnitSphereProd E sends an additive Haar measure μ
to the product of μ.toSphere and MeasureTheory.Measure.volumeIoiPow (dim E - 1),
where dim E = Module.finrank ℝ E is the dimension of E.