An integration structure on a differential form space supporting Stokes' theorem: provides a top dimension $n$, a wedge-pairing $\langle \alpha, \beta \rangle$ on $p$-forms, an integral $\int : \Omega^n \to \mathbb{R}$, and the Leibniz/integration-by-parts identity $\int (d\alpha) \wedge \beta = (-1)^{p+1} \int \alpha \wedge d\beta$.
- n : ℕ
- wedge_star_linear_left (p : ℕ) (r : ℝ) (α₁ α₂ β : Ω p) : self.wedge_star p (r • α₁ + α₂) β = r • self.wedge_star p α₁ β + self.wedge_star p α₂ β
- wedge_star_linear_right (p : ℕ) (r : ℝ) (α β₁ β₂ : Ω p) : self.wedge_star p α (r • β₁ + β₂) = r • self.wedge_star p α β₁ + self.wedge_star p α β₂
- leibniz_rule (p : ℕ) (α : Ω p) (β : Ω (p + 1)) : self.integrate (self.wedge_star (p + 1) (DifferentialFormSpace.d VF α) β) = (-1) ^ (p + 1) • self.integrate (self.wedge_star_d p α β)
Instances For
The $L^2$ inner product on $p$-forms induced by the Hodge-star pairing: $\langle \alpha, \beta \rangle = \int \alpha \wedge \star \beta$.
Instances For
Linearity of the inner product in the first argument: $\langle r\alpha_1 + \alpha_2, \beta \rangle = r\langle \alpha_1, \beta \rangle + \langle \alpha_2, \beta \rangle$.
Adjointness from Stokes' theorem: $\langle d\alpha, \beta \rangle = (-1)^{p+1} \int \alpha \wedge d\beta$, identifying $d$ as (up to sign) the formal adjoint to itself in the pairing.