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TauCeti.Analysis.Complex.Wirtinger.Weak

Weak conjugate Wirtinger derivatives #

HasWeakConjWirtingerDerivOn μ Ω u g expresses \bar∂u = g by integration by parts against real smooth compactly supported test functions. The normalization is \bar∂ = (∂₁ + I ∂ᵢ)/2. This does not require either real first derivative of u to be represented by a function.

The codomain is complete and both functions are locally integrable, preventing the totalized Bochner integral from making the defining identity vacuous. With a Haar measure the identity is the distributional equation; for a general measure it is the corresponding adjoint relation.

Main results #

The relation is local, complex-linear, invariant under almost-everywhere replacement and compatible with continuous complex-linear maps. Its value is unique almost everywhere. hasWeakConjWirtingerDerivOn_of_hasWeakLineDerivOn and HasWeakFDerivOn.hasWeakConjWirtingerDerivOn compare it with the native real weak derivatives, and HasWeakConjWirtingerDerivOn.weakLineDeriv differentiates the equation in a real direction. hasWeakConjWirtingerDerivOn_of_contDiffOn compares it with the classical normalized operator; for real C¹ maps, its vanishing is equivalent to holomorphy. Every holomorphic map solves the distributional equation. hasWeakConjWirtingerDerivOn_conj computes the weak derivative of conjugation as 1, which rules out an almost-everywhere equal holomorphic representative on nonempty open sets.

References #

The normalized distributional equation \bar∂u = g, relative to μ, with locally integrable source and derivative and a complete codomain. Real tests suffice for a complex-linear equation.

Instances For

    The defining conditions, usable without unfolding the sealed definition.

    The codomain of a weak conjugate Wirtinger derivative is complete.

    The weak conjugate Wirtinger derivative is locally integrable.

    Integration by parts for the normalized conjugate Wirtinger derivative.

    Weak conjugate Wirtinger differentiation restricts to smaller open sets.

    @[simp]

    The zero function has weak conjugate Wirtinger derivative zero.

    Weak conjugate Wirtinger differentiation commutes with negation.

    Weak conjugate Wirtinger differentiation commutes with addition.

    Weak conjugate Wirtinger differentiation commutes with subtraction.

    theorem TauCeti.HasWeakConjWirtingerDerivOn.clm_comp {F : Type u_1} [NormedAddCommGroup F] [NormedSpace ℂ F] {μ : MeasureTheory.Measure ℂ} {Ω : TopologicalSpace.Opens ℂ} {u g : ℂ → F} {G : Type u_2} [NormedAddCommGroup G] [NormedSpace ℂ G] [CompleteSpace G] (h : HasWeakConjWirtingerDerivOn μ Ω u g) (L : F →L[ℂ] G) :
    HasWeakConjWirtingerDerivOn μ Ω (fun (z : ℂ) => L (u z)) fun (z : ℂ) => L (g z)

    A complex continuous linear map commutes with the weak conjugate Wirtinger derivative.

    Weak conjugate Wirtinger differentiation is complex-linear.

    Almost-everywhere replacement on the open set preserves the source of a weak derivative.

    Almost-everywhere replacement preserves the weak conjugate Wirtinger derivative.

    The weak conjugate Wirtinger derivative is unique almost everywhere on the open set.

    The two weak real partial derivatives combine to the normalized weak \bar∂ derivative.

    A weak Fréchet derivative determines the weak conjugate Wirtinger derivative.

    The classical conjugate Wirtinger derivative of a C¹ function is its weak derivative.

    Conjugation has normalized weak \bar∂ derivative 1, fixing both its sign and factor.

    For a function of class C¹ over ℝ, the weak equation \bar∂u=0 is precisely holomorphy.

    Every holomorphic function with Banach coefficients solves the distributional equation.

    Conjugation cannot agree almost everywhere with a holomorphic function on a nonempty open set: its weak \bar∂ derivative is 1, while a holomorphic representative has derivative 0.

    A weak directional derivative of a solution of \bar∂u = f solves the differentiated equation \bar∂(∂ᵥu) = ∂ᵥf. No other derivative of u or f is assumed.