Bilinear pairings of two directional derivatives of a compactly supported map #
For a compactly supported C² map u on a finite-dimensional real space and a continuous
bilinear map B, the integral of B (∂_v u) (∂_w u) against a Haar measure does not change when
the two directions are exchanged. Integrating by parts in the direction w turns it into
-∫ B (∂_w ∂_v u) u, and the exchanged integral into -∫ B (∂_v ∂_w u) u; the two agree because
the second derivative is symmetric.
Consequently the integral vanishes whenever B is alternating. That is the vanishing of the
integral over the whole space of the pullback of a constant two-form along a compactly supported
map — the "null Lagrangian" phenomenon: for a map from the plane to the plane, with B the
standard area form and the two coordinate directions, the integrand is the Jacobian determinant.
It is what makes the energy of a compactly supported map into a symplectic vector space equal the
square of the L² norm of its Cauchy--Riemann defect.
Main results #
TauCeti.integral_bilinear_fderiv_apply_comm: the integral ofB (∂_v u) (∂_w u)is symmetric in the two directions, andTauCeti.integral_bilinForm_fderiv_apply_commits form for a bilinear form on a finite-dimensional space.TauCeti.integral_bilinForm_fderiv_apply_eq_zero_of_isAlt: for an alternating bilinear form the integral vanishes.
References #
- Sébastien Gouëzel,
Mathlib/Analysis/Calculus/LineDeriv/IntegrationByParts.lean, theoremintegral_bilinear_fderiv_right_eq_neg_left_of_integrable: the integration by parts in a single direction that every proof here is built on.
Exchanging the two differentiation directions does not change the integral of a continuous
bilinear pairing of two directional derivatives of a compactly supported C² map.
Exchanging the two differentiation directions does not change the integral of a bilinear form
evaluated on two directional derivatives of a compactly supported C² map into a
finite-dimensional space.
The integral of an alternating bilinear form evaluated on two directional derivatives of a
compactly supported C² map vanishes: the pullback of a constant two-form along a compactly
supported map integrates to zero.