Combine a geometric-series integral, a Jacobian and symmetry to prove the Basel sum.
This page uses the chapter's tools to prove Euler's result
∑n≥11/n2=π2/6. The p-series
test with p=2
shows that the series converges; a double integral finds its value.
Let Ω be a region in (x,y)-coordinates and let Φ be a region
in (u,v)-coordinates. Assume that f is integrable on Ω, that g
is C1 on Φ, that Φ can be split into finitely many pieces on
which g is one-to-one with non-overlapping interiors and that the Jacobian
is nonzero away from boundary or other exceptional sets of area zero. The
images of those pieces must cover Ω once, apart from boundaries of area
zero; otherwise the transformed integral can omit or count part of the region
more than once. If a map covers the target with multiplicity, split the
parameter region into one-to-one pieces (or account for that multiplicity)
before applying the formula.
Then
Multiplying two copies of this identity and using Fubini on the unit square
gives
(n+1)21=∫01∫01(xy)ndxdy.
To sum over n, use the geometric series: for 0≤x,y<1,
n=0∑∞(xy)n=1−xy1.
The finite geometric sums are nonnegative and increase pointwise, so monotone
convergence justifies taking their limit under the integral.
The integrand 1/(1−xy) is singular only at the corner (1,1), but it is
unbounded in every neighbourhood of that corner. The integral is therefore
improper, defined as the monotone limit over bounded truncations. The corner
has zero area, but the blow-up near it cannot be ignored.
Summing the identities over n≥0 therefore gives
S:=n=1∑∞n21=∬[0,1]21−xy1dxdy.
For the same reason, the proof applies the change-of-variables theorem on
compact subregions that stay away from (1,1) and then removes the
truncation by monotone convergence. The transformed integrals are understood
as the corresponding improper limits.
Each piece now needs one trigonometric substitution. The first uses
u=sinθ; the second uses u=cosθ, so that the inverse tangent
simplifies by the half-angle identity.
For the second piece, let u=cosθ, so
0≤θ≤π/3. As u runs from 1/2 to 1, θ runs from
π/3 to 0; flipping the limits removes the minus sign from
du=−sinθdθ. The ratio in the inverse tangent is