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
Equations
- ⋯ = ⋯
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
Equations
- ⋯ = ⋯
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
.